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	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Charged_Ring&amp;diff=38742</id>
		<title>Charged Ring</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Charged_Ring&amp;diff=38742"/>
		<updated>2020-04-22T03:01:03Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
Charges may be arranged in a variety of ways. When points are uniformly distributed a finite distance away from some point, which we define as the origin, we call this curve as a ring. We can position a [[Point Charge]] at every point upon this ring. To analyze this continuous arrangement of charges, we say that their individual contributions are infinitesimally small, and then sum each of these contributions together to arrive at the electric field produced by this charge distribution. We can compute the net electric field of this charge distribution with Coulomb&#039;s Law and by applying integration principles. The ring field can also be used to calculate the electric field of a [[Charged Disk]].&lt;br /&gt;
&lt;br /&gt;
==A Mathematical Model==&lt;br /&gt;
&lt;br /&gt;
This mathematical model is based on the individual [[Electric Field]] contributions of a number of point charges, each of which is defined by&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E} = \frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Do not forget this equation&#039;&#039;&#039;. This equation must be memorized as it isn&#039;t given on the formula sheet. &lt;br /&gt;
&lt;br /&gt;
We also say that this vector field is a member of a linear space of vectors. This is to say that we can apply the [[Superposition Principle]] meaning that we can sum any number of these electric field vectors and obtain another vector which is the electric field vector contributed by those charges. When we continuously sum all of the vectors produced by these charges, we get the electric field produced by the entire arrangement of charges.&lt;br /&gt;
&lt;br /&gt;
[[File:red_ring.png|400px|thumb|Figure 1: diagram of a charged ring]]&lt;br /&gt;
&lt;br /&gt;
The diagram above shows the electric field due to one infinitesimal piece of the ring, &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;. In order to avoid rigorous computations, we can see that the electric field of the charges cancels out in the vertical direction. Only the horizontal component will remain. For an observation location that is on the symmetry axis as the ring, the other two components will be zero. If the observation location were off axis, then it would be very different requiring more math. Since each piece, &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;, contributes a &amp;lt;math&amp;gt;d\vec{E}&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;\frac{1}{4\pi\epsilon_{0}}\frac{dq}{|\vec{d}|^{2}}\hat{d}&amp;lt;/math&amp;gt;, we can compute the horizontal component by multiplying the magnitude of &amp;lt;math&amp;gt;d\vec{E}&amp;lt;/math&amp;gt; with &amp;lt;math&amp;gt;\cos{θ}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;|d\vec{E}_{z}| = \frac{1}{4\pi\epsilon_{0}}\frac{dq}{r^2 + z^2}\cos{θ} = \frac{1}{4\pi\epsilon_{0}}\frac{dq}{r^2 + z^2}\frac{z}{(r^2 + z^2)^\frac{1}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Now we integrate to sum all the electric field contributions of each infinitesimal &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}_{z} = \frac{1}{4\pi\epsilon_{0}}\frac{z}{(r^2 + z^2)^\frac{3}{2}}\int_{}^{} dq = \frac{1}{4\pi\epsilon_{0}}\frac{Qz}{(r^2 + z^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
As a reminder, this is the equation given on the formula sheet. It &#039;&#039;&#039;only&#039;&#039;&#039; works when the location at which the field is being measured is along the &amp;lt;math&amp;gt;{z}&amp;lt;/math&amp;gt; axis. However, the equation for it being off axis is not given on the equation sheet. That requires a separate and more difficult integration. Typically, the only way this would be asked on a test is to set up an equation that would be integrated that requires you to find a new &amp;lt;math&amp;gt;dQ&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
See below for a more rigorous derivation.&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/glowscript/707d492e19 This simulation] shows the result of the computation for a ring composed of 2000 electrons. This is why the vector is pointing into the ring rather than out of the ring, which would happen for a ring composed of positively charged points.&lt;br /&gt;
&lt;br /&gt;
==Rigorous Derivation==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Define shape characteristics of the ring===&lt;br /&gt;
&lt;br /&gt;
The ring has some finite charge.&lt;br /&gt;
&lt;br /&gt;
We see that this arrangement is circular, so a coordinate system with which we can define radial and angular coordinates would be useful. Naturally, this would be the polar coordinate system.&lt;br /&gt;
&lt;br /&gt;
We also see that all charge is uniformly distributed some finite distance R from the center of the ring. It would be useful to let the center of the ring be the origin of our coordinate axes.&lt;br /&gt;
&lt;br /&gt;
Here is a reasonable arrangement for this charged ring.&lt;br /&gt;
&lt;br /&gt;
[[File:blue_graph.png|400px|thumb|Figure 2: defining a coordinate system about a charged ring]]&lt;br /&gt;
&lt;br /&gt;
Since all charge is concentrated upon the edge of the circle, we can consider our charge distribution to be invariant with respect to radial distance. However, we do see that our charge distribution is the function of theta.&lt;br /&gt;
&lt;br /&gt;
===Compute charge distribution function===&lt;br /&gt;
Let us call the charge distribution as &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\sigma&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We have a charge distributed on the edge of the circle, so&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \sigma=\frac{Q}{2\pi} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;Q&amp;lt;/math&amp;gt; represents the charge of the ring.&lt;br /&gt;
&lt;br /&gt;
What this equation means is that the charge is uniformly distributed along each unit of angular length. In this way, it is called angular charge density.&lt;br /&gt;
&lt;br /&gt;
===Compute infinitesimal charge contribution===&lt;br /&gt;
&lt;br /&gt;
Let us consider an infinitesimal section of the ring which contains exactly one point charge. The dimension of this section is given by &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;d\theta&amp;lt;/math&amp;gt; which is the infinitesimal angular size. So, the infinitesimal charge contribution, &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;dQ&amp;lt;/math&amp;gt;, is&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; dQ = \frac{Q}{2\pi}d\theta &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Compute infinitesimal electric field contribution===&lt;br /&gt;
&lt;br /&gt;
Let us define some arbitrary location at which we are observing this ring of charge.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{r} = x\hat{x}+y\hat{y} + z\hat{z} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
in polar coordinates, we see this becomes&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{r} = Rcos(\theta)\hat{x} + Rsin(\theta)\hat{y} + z\hat{z} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Recall that both sine and cosine are periodic with the period of &amp;lt;math&amp;gt;2\pi &amp;lt;/math&amp;gt;. This will become important later.&lt;br /&gt;
&lt;br /&gt;
The magnitude of this vector is&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; |\vec{r}| = \sqrt{R^{2}+z^{2}} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
owing to the usage of the Pythagorean trigonometric identity.&lt;br /&gt;
&lt;br /&gt;
Now, we have what we need to write the electric field vector contributed by each piece of the ring of charge. Let this vector field piece be &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;d\vec{E}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; d\vec{E}=\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r}=\frac{1}{4\pi\epsilon_{0}}\frac{dQ}{(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Compute electric field vector===&lt;br /&gt;
&lt;br /&gt;
So, now all that is left is to sum everything up. We are summing over the circumference of a circle, so our path is defined by &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;0\leq\theta\leq 2\pi &amp;lt;/math&amp;gt;. Let us now set up our integral.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}=\int_{0}^{2\pi}\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} d\theta=\int_{0}^{2\pi}\frac{1}{4\pi\epsilon_{0}}\frac{Q}{2\pi(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z})d\theta&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Since both sine and cosine are &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;2\pi&amp;lt;/math&amp;gt; periodic functions, the &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;x&amp;lt;/math&amp;gt; and &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;y&amp;lt;/math&amp;gt; components of &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\vec{E}&amp;lt;/math&amp;gt; go to &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\vec{0}&amp;lt;/math&amp;gt;, which is very convenient. The result is&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{E}=\frac{1}{4\pi\epsilon_{0}}\frac{Qz}{(z^{2}+R^{2})^{3/2}}\hat{z} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
===Remark===&lt;br /&gt;
&lt;br /&gt;
If the path we are interested in is over a half circle, third-circle or quarter-circle, or indeed any circular section, simply adjust the bounds of integration and the charge density to the ones required by the curve of interest.&lt;br /&gt;
&lt;br /&gt;
==Example Problems==&lt;br /&gt;
&lt;br /&gt;
===Easy===&lt;br /&gt;
&lt;br /&gt;
1.) Find the function &amp;lt;math&amp;gt;E(x)&amp;lt;/math&amp;gt; that represents the magnitude of the electric field along the center axis due to a uniformly charged ring of radius 0.04 m with total charge 8 C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We can use the derived formula for the electric field due to a charged ring. Only the horizontal components of the electric field will remain as the rest will cancel out.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;E(x) = \frac{1}{4\pi\epsilon_{0}}\frac{(8 C)*x}{((0.04 m)^2 + x^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
2.) A uniformly charged ring of radius 10.0 cm has a total charge of 91.0 µC. Find the electric field on the axis of the ring at the following distances from the center of the ring.&lt;br /&gt;
&lt;br /&gt;
a. 1 cm &lt;br /&gt;
&lt;br /&gt;
b. 5 cm &lt;br /&gt;
&lt;br /&gt;
c. 30 cm &lt;br /&gt;
&lt;br /&gt;
d. 100 cm&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Use the derived formula, and convert the given distances into meters and the charge into Coulombs. Plug these into &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;E(x) = \frac{1}{4\pi\epsilon_{0}}\frac{Q*x}{(x^2 + R^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
a. 8.069e6 N/C&lt;br /&gt;
&lt;br /&gt;
b. 29.3e6 N/C&lt;br /&gt;
&lt;br /&gt;
c. 7.76e6 N/C&lt;br /&gt;
&lt;br /&gt;
d. 8.06e5 N/C&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Find the electric field at a distance &amp;lt;math&amp;gt;z&amp;lt;/math&amp;gt; along the center axis away from a uniformly charged semicircular ring of radius R and total charge Q.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We can tweak the same integral for a uniformly charged ring by changing the limits of integration.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}=\int_{0}^{\pi}\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} d\theta=\int_{0}^{\pi}\frac{1}{4\pi\epsilon_{0}}\frac{Q}{\pi(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z})d\theta&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E} = \frac{1}{4\pi\epsilon_{0}}\frac{Q}{\pi(R^{2}+z^{2})^{3/2}}(0\hat{x}+2R\hat{y}+{\pi}z\hat{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Added by AYESHA AHUJA SPRING 2020&lt;br /&gt;
&lt;br /&gt;
The first known time when charged rings were utilized to describe electromagnetism was during Faraday’s discovery of electrical induction. To conduct his experiments, Faraday used a ring made of iron that was attached to a battery. When this makeshift circuit was turned on it manipulated a compass needle by deflecting it. He showcased an induced current in the ring.&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
Edited by AYESHA AHUJA Spring 2020 &lt;br /&gt;
&lt;br /&gt;
The idea of charge density is somewhat analogous to the idea of the mass density, which is useful in a variety of contexts, including the computation of the center of mass, the first and second moments of mass, which are useful in statics and rigid body dynamics. Instead of computing the uniform distribution of the mass of this ring, we are computing the uniform distribution of charge. This concept is also useful in visualizing what happens within a wire in a steady state circuit. The wire can be viewed to be a continuous length of rings of charge, which act as a channel through which electrons are transported, and that the electric field of these rings of charge pushes the electrons within the wire.&lt;br /&gt;
&lt;br /&gt;
It is also important in the context of Maxwell&#039;s equations, specifically in Gauss&#039;s Law and in the Maxwell-Faraday equation, which are concerned with electron flux and induced fields, respectively.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Charged Rod]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Disk]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Spherical Shell]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Capacitor]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&amp;quot;Electric Field on the Axis of a Ring of Charge&amp;quot;.  University of Delaware Physics Library.  Adapted from Stephen Kevan&#039;s lecture on Electric Fields and Charge Distribution.  April 8, 1996.  http://www.physics.udel.edu/~watson/phys208/exercises/kevan/efield1.html&lt;br /&gt;
&lt;br /&gt;
Chabay, R., &amp;amp; Sherwood, B. (2015). Matter and Interactions (4th ed., Vol. 2, pp. 597-599). Wiley.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
All images produced by the author&lt;br /&gt;
&lt;br /&gt;
==External Links==&lt;br /&gt;
&lt;br /&gt;
https://www.youtube.com/watch?v=80mM3kSTZcE&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elelin.html&lt;br /&gt;
&lt;br /&gt;
http://www.physics.udel.edu/~watson/phys208/exercises/kevan/efield1.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Electric Fields]]&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Charged_Ring&amp;diff=38741</id>
		<title>Charged Ring</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Charged_Ring&amp;diff=38741"/>
		<updated>2020-04-22T03:00:51Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
Charges may be arranged in a variety of ways. When points are uniformly distributed a finite distance away from some point, which we define as the origin, we call this curve as a ring. We can position a [[Point Charge]] at every point upon this ring. To analyze this continuous arrangement of charges, we say that their individual contributions are infinitesimally small, and then sum each of these contributions together to arrive at the electric field produced by this charge distribution. We can compute the net electric field of this charge distribution with Coulomb&#039;s Law and by applying integration principles. The ring field can also be used to calculate the electric field of a [[Charged Disk]].&lt;br /&gt;
&lt;br /&gt;
==A Mathematical Model==&lt;br /&gt;
&lt;br /&gt;
This mathematical model is based on the individual [[Electric Field]] contributions of a number of point charges, each of which is defined by&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E} = \frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Do not forget this equation&#039;&#039;&#039;. This equation must be memorized as it isn&#039;t given on the formula sheet. &lt;br /&gt;
&lt;br /&gt;
We also say that this vector field is a member of a linear space of vectors. This is to say that we can apply the [[Superposition Principle]] meaning that we can sum any number of these electric field vectors and obtain another vector which is the electric field vector contributed by those charges. When we continuously sum all of the vectors produced by these charges, we get the electric field produced by the entire arrangement of charges.&lt;br /&gt;
&lt;br /&gt;
[[File:red_ring.png|400px|thumb|Figure 1: diagram of a charged ring]]&lt;br /&gt;
&lt;br /&gt;
The diagram above shows the electric field due to one infinitesimal piece of the ring, &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;. In order to avoid rigorous computations, we can see that the electric field of the charges cancels out in the vertical direction. Only the horizontal component will remain. For an observation location that is on the symmetry axis as the ring, the other two components will be zero. If the observation location were off axis, then it would be very different requiring more math. Since each piece, &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;, contributes a &amp;lt;math&amp;gt;d\vec{E}&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;\frac{1}{4\pi\epsilon_{0}}\frac{dq}{|\vec{d}|^{2}}\hat{d}&amp;lt;/math&amp;gt;, we can compute the horizontal component by multiplying the magnitude of &amp;lt;math&amp;gt;d\vec{E}&amp;lt;/math&amp;gt; with &amp;lt;math&amp;gt;\cos{θ}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;|d\vec{E}_{z}| = \frac{1}{4\pi\epsilon_{0}}\frac{dq}{r^2 + z^2}\cos{θ} = \frac{1}{4\pi\epsilon_{0}}\frac{dq}{r^2 + z^2}\frac{z}{(r^2 + z^2)^\frac{1}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Now we integrate to sum all the electric field contributions of each infinitesimal &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}_{z} = \frac{1}{4\pi\epsilon_{0}}\frac{z}{(r^2 + z^2)^\frac{3}{2}}\int_{}^{} dq = \frac{1}{4\pi\epsilon_{0}}\frac{Qz}{(r^2 + z^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
As a reminder, this is the equation given on the formula sheet. It &#039;&#039;&#039;only&#039;&#039;&#039; works when the location at which the field is being measured is along the &amp;lt;math&amp;gt;{z}&amp;lt;/math&amp;gt; axis. However, the equation for it being off axis is not given on the equation sheet. That requires a separate and more difficult integration. Typically, the only way this would be asked on a test is to set up an equation that would be integrated that requires you to find a new &amp;lt;math&amp;gt;dQ&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
See below for a more rigorous derivation.&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/glowscript/707d492e19 This simulation] shows the result of the computation for a ring composed of 2000 electrons. This is why the vector is pointing into the ring rather than out of the ring, which would happen for a ring composed of positively charged points.&lt;br /&gt;
&lt;br /&gt;
==Rigorous Derivation==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Define shape characteristics of the ring===&lt;br /&gt;
&lt;br /&gt;
The ring has some finite charge.&lt;br /&gt;
&lt;br /&gt;
We see that this arrangement is circular, so a coordinate system with which we can define radial and angular coordinates would be useful. Naturally, this would be the polar coordinate system.&lt;br /&gt;
&lt;br /&gt;
We also see that all charge is uniformly distributed some finite distance R from the center of the ring. It would be useful to let the center of the ring be the origin of our coordinate axes.&lt;br /&gt;
&lt;br /&gt;
Here is a reasonable arrangement for this charged ring.&lt;br /&gt;
&lt;br /&gt;
[[File:blue_graph.png|400px|thumb|Figure 2: defining a coordinate system about a charged ring]]&lt;br /&gt;
&lt;br /&gt;
Since all charge is concentrated upon the edge of the circle, we can consider our charge distribution to be invariant with respect to radial distance. However, we do see that our charge distribution is the function of theta.&lt;br /&gt;
&lt;br /&gt;
===Compute charge distribution function===&lt;br /&gt;
Let us call the charge distribution as &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\sigma&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We have a charge distributed on the edge of the circle, so&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \sigma=\frac{Q}{2\pi} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;Q&amp;lt;/math&amp;gt; represents the charge of the ring.&lt;br /&gt;
&lt;br /&gt;
What this equation means is that the charge is uniformly distributed along each unit of angular length. In this way, it is called angular charge density.&lt;br /&gt;
&lt;br /&gt;
===Compute infinitesimal charge contribution===&lt;br /&gt;
&lt;br /&gt;
Let us consider an infinitesimal section of the ring which contains exactly one point charge. The dimension of this section is given by &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;d\theta&amp;lt;/math&amp;gt; which is the infinitesimal angular size. So, the infinitesimal charge contribution, &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;dQ&amp;lt;/math&amp;gt;, is&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; dQ = \frac{Q}{2\pi}d\theta &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Compute infinitesimal electric field contribution===&lt;br /&gt;
&lt;br /&gt;
Let us define some arbitrary location at which we are observing this ring of charge.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{r} = x\hat{x}+y\hat{y} + z\hat{z} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
in polar coordinates, we see this becomes&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{r} = Rcos(\theta)\hat{x} + Rsin(\theta)\hat{y} + z\hat{z} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Recall that both sine and cosine are periodic with the period of &amp;lt;math&amp;gt;2\pi &amp;lt;/math&amp;gt;. This will become important later.&lt;br /&gt;
&lt;br /&gt;
The magnitude of this vector is&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; |\vec{r}| = \sqrt{R^{2}+z^{2}} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
owing to the usage of the Pythagorean trigonometric identity.&lt;br /&gt;
&lt;br /&gt;
Now, we have what we need to write the electric field vector contributed by each piece of the ring of charge. Let this vector field piece be &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;d\vec{E}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; d\vec{E}=\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r}=\frac{1}{4\pi\epsilon_{0}}\frac{dQ}{(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Compute electric field vector===&lt;br /&gt;
&lt;br /&gt;
So, now all that is left is to sum everything up. We are summing over the circumference of a circle, so our path is defined by &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;0\leq\theta\leq 2\pi &amp;lt;/math&amp;gt;. Let us now set up our integral.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}=\int_{0}^{2\pi}\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} d\theta=\int_{0}^{2\pi}\frac{1}{4\pi\epsilon_{0}}\frac{Q}{2\pi(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z})d\theta&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Since both sine and cosine are &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;2\pi&amp;lt;/math&amp;gt; periodic functions, the &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;x&amp;lt;/math&amp;gt; and &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;y&amp;lt;/math&amp;gt; components of &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\vec{E}&amp;lt;/math&amp;gt; go to &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\vec{0}&amp;lt;/math&amp;gt;, which is very convenient. The result is&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{E}=\frac{1}{4\pi\epsilon_{0}}\frac{Qz}{(z^{2}+R^{2})^{3/2}}\hat{z} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
===Remark===&lt;br /&gt;
&lt;br /&gt;
If the path we are interested in is over a half circle, third-circle or quarter-circle, or indeed any circular section, simply adjust the bounds of integration and the charge density to the ones required by the curve of interest.&lt;br /&gt;
&lt;br /&gt;
==Example Problems==&lt;br /&gt;
&lt;br /&gt;
===Easy===&lt;br /&gt;
&lt;br /&gt;
1.) Find the function &amp;lt;math&amp;gt;E(x)&amp;lt;/math&amp;gt; that represents the magnitude of the electric field along the center axis due to a uniformly charged ring of radius 0.04 m with total charge 8 C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We can use the derived formula for the electric field due to a charged ring. Only the horizontal components of the electric field will remain as the rest will cancel out.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;E(x) = \frac{1}{4\pi\epsilon_{0}}\frac{(8 C)*x}{((0.04 m)^2 + x^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
2.) A uniformly charged ring of radius 10.0 cm has a total charge of 91.0 µC. Find the electric field on the axis of the ring at the following distances from the center of the ring.&lt;br /&gt;
&lt;br /&gt;
a. 1 cm &lt;br /&gt;
&lt;br /&gt;
b. 5 cm &lt;br /&gt;
&lt;br /&gt;
c. 30 cm &lt;br /&gt;
&lt;br /&gt;
d. 100 cm&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Use the derived formula, and convert the given distances into meters and the charge into Coulombs. Plug these into &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;E(x) = \frac{1}{4\pi\epsilon_{0}}\frac{Q*x}{(x^2 + R^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
a. 8.069e6 N/C&lt;br /&gt;
&lt;br /&gt;
b. 29.3e6 N/C&lt;br /&gt;
&lt;br /&gt;
c. 7.76e6 N/C&lt;br /&gt;
&lt;br /&gt;
d. 8.06e5 N/C&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Find the electric field at a distance &amp;lt;math&amp;gt;z&amp;lt;/math&amp;gt; along the center axis away from a uniformly charged semicircular ring of radius R and total charge Q.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We can tweak the same integral for a uniformly charged ring by changing the limits of integration.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}=\int_{0}^{\pi}\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} d\theta=\int_{0}^{\pi}\frac{1}{4\pi\epsilon_{0}}\frac{Q}{\pi(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z})d\theta&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E} = \frac{1}{4\pi\epsilon_{0}}\frac{Q}{\pi(R^{2}+z^{2})^{3/2}}(0\hat{x}+2R\hat{y}+{\pi}z\hat{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Added by AYESHA AHUJA SPRING 2020&lt;br /&gt;
&lt;br /&gt;
The first known time when charged rings were utilized to describe electromagnetism was during Faraday’s discovery of electrical induction. To conduct his experiments, Faraday used a ring made of iron that was attached to a battery. When this makeshift circuit was turned on it manipulated a compass needle by deflecting it. He showcased an induced current in the ring.&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
edited by AYESHA AHUJA Spring 2020 &lt;br /&gt;
&lt;br /&gt;
The idea of charge density is somewhat analogous to the idea of the mass density, which is useful in a variety of contexts, including the computation of the center of mass, the first and second moments of mass, which are useful in statics and rigid body dynamics. Instead of computing the uniform distribution of the mass of this ring, we are computing the uniform distribution of charge. This concept is also useful in visualizing what happens within a wire in a steady state circuit. The wire can be viewed to be a continuous length of rings of charge, which act as a channel through which electrons are transported, and that the electric field of these rings of charge pushes the electrons within the wire.&lt;br /&gt;
&lt;br /&gt;
It is also important in the context of Maxwell&#039;s equations, specifically in Gauss&#039;s Law and in the Maxwell-Faraday equation, which are concerned with electron flux and induced fields, respectively.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Charged Rod]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Disk]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Spherical Shell]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Capacitor]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&amp;quot;Electric Field on the Axis of a Ring of Charge&amp;quot;.  University of Delaware Physics Library.  Adapted from Stephen Kevan&#039;s lecture on Electric Fields and Charge Distribution.  April 8, 1996.  http://www.physics.udel.edu/~watson/phys208/exercises/kevan/efield1.html&lt;br /&gt;
&lt;br /&gt;
Chabay, R., &amp;amp; Sherwood, B. (2015). Matter and Interactions (4th ed., Vol. 2, pp. 597-599). Wiley.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
All images produced by the author&lt;br /&gt;
&lt;br /&gt;
==External Links==&lt;br /&gt;
&lt;br /&gt;
https://www.youtube.com/watch?v=80mM3kSTZcE&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elelin.html&lt;br /&gt;
&lt;br /&gt;
http://www.physics.udel.edu/~watson/phys208/exercises/kevan/efield1.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Electric Fields]]&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Charged_Ring&amp;diff=38740</id>
		<title>Charged Ring</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Charged_Ring&amp;diff=38740"/>
		<updated>2020-04-22T02:57:36Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
Charges may be arranged in a variety of ways. When points are uniformly distributed a finite distance away from some point, which we define as the origin, we call this curve as a ring. We can position a [[Point Charge]] at every point upon this ring. To analyze this continuous arrangement of charges, we say that their individual contributions are infinitesimally small, and then sum each of these contributions together to arrive at the electric field produced by this charge distribution. We can compute the net electric field of this charge distribution with Coulomb&#039;s Law and by applying integration principles. The ring field can also be used to calculate the electric field of a [[Charged Disk]].&lt;br /&gt;
&lt;br /&gt;
==A Mathematical Model==&lt;br /&gt;
&lt;br /&gt;
This mathematical model is based on the individual [[Electric Field]] contributions of a number of point charges, each of which is defined by&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E} = \frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Do not forget this equation&#039;&#039;&#039;. This equation must be memorized as it isn&#039;t given on the formula sheet. &lt;br /&gt;
&lt;br /&gt;
We also say that this vector field is a member of a linear space of vectors. This is to say that we can apply the [[Superposition Principle]] meaning that we can sum any number of these electric field vectors and obtain another vector which is the electric field vector contributed by those charges. When we continuously sum all of the vectors produced by these charges, we get the electric field produced by the entire arrangement of charges.&lt;br /&gt;
&lt;br /&gt;
[[File:red_ring.png|400px|thumb|Figure 1: diagram of a charged ring]]&lt;br /&gt;
&lt;br /&gt;
The diagram above shows the electric field due to one infinitesimal piece of the ring, &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;. In order to avoid rigorous computations, we can see that the electric field of the charges cancels out in the vertical direction. Only the horizontal component will remain. For an observation location that is on the symmetry axis as the ring, the other two components will be zero. If the observation location were off axis, then it would be very different requiring more math. Since each piece, &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;, contributes a &amp;lt;math&amp;gt;d\vec{E}&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;\frac{1}{4\pi\epsilon_{0}}\frac{dq}{|\vec{d}|^{2}}\hat{d}&amp;lt;/math&amp;gt;, we can compute the horizontal component by multiplying the magnitude of &amp;lt;math&amp;gt;d\vec{E}&amp;lt;/math&amp;gt; with &amp;lt;math&amp;gt;\cos{θ}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;|d\vec{E}_{z}| = \frac{1}{4\pi\epsilon_{0}}\frac{dq}{r^2 + z^2}\cos{θ} = \frac{1}{4\pi\epsilon_{0}}\frac{dq}{r^2 + z^2}\frac{z}{(r^2 + z^2)^\frac{1}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Now we integrate to sum all the electric field contributions of each infinitesimal &amp;lt;math&amp;gt;dq&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}_{z} = \frac{1}{4\pi\epsilon_{0}}\frac{z}{(r^2 + z^2)^\frac{3}{2}}\int_{}^{} dq = \frac{1}{4\pi\epsilon_{0}}\frac{Qz}{(r^2 + z^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
As a reminder, this is the equation given on the formula sheet. It &#039;&#039;&#039;only&#039;&#039;&#039; works when the location at which the field is being measured is along the &amp;lt;math&amp;gt;{z}&amp;lt;/math&amp;gt; axis. However, the equation for it being off axis is not given on the equation sheet. That requires a separate and more difficult integration. Typically, the only way this would be asked on a test is to set up an equation that would be integrated that requires you to find a new &amp;lt;math&amp;gt;dQ&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
See below for a more rigorous derivation.&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/glowscript/707d492e19 This simulation] shows the result of the computation for a ring composed of 2000 electrons. This is why the vector is pointing into the ring rather than out of the ring, which would happen for a ring composed of positively charged points.&lt;br /&gt;
&lt;br /&gt;
==Rigorous Derivation==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Define shape characteristics of the ring===&lt;br /&gt;
&lt;br /&gt;
The ring has some finite charge.&lt;br /&gt;
&lt;br /&gt;
We see that this arrangement is circular, so a coordinate system with which we can define radial and angular coordinates would be useful. Naturally, this would be the polar coordinate system.&lt;br /&gt;
&lt;br /&gt;
We also see that all charge is uniformly distributed some finite distance R from the center of the ring. It would be useful to let the center of the ring be the origin of our coordinate axes.&lt;br /&gt;
&lt;br /&gt;
Here is a reasonable arrangement for this charged ring.&lt;br /&gt;
&lt;br /&gt;
[[File:blue_graph.png|400px|thumb|Figure 2: defining a coordinate system about a charged ring]]&lt;br /&gt;
&lt;br /&gt;
Since all charge is concentrated upon the edge of the circle, we can consider our charge distribution to be invariant with respect to radial distance. However, we do see that our charge distribution is the function of theta.&lt;br /&gt;
&lt;br /&gt;
===Compute charge distribution function===&lt;br /&gt;
Let us call the charge distribution as &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\sigma&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We have a charge distributed on the edge of the circle, so&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \sigma=\frac{Q}{2\pi} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;Q&amp;lt;/math&amp;gt; represents the charge of the ring.&lt;br /&gt;
&lt;br /&gt;
What this equation means is that the charge is uniformly distributed along each unit of angular length. In this way, it is called angular charge density.&lt;br /&gt;
&lt;br /&gt;
===Compute infinitesimal charge contribution===&lt;br /&gt;
&lt;br /&gt;
Let us consider an infinitesimal section of the ring which contains exactly one point charge. The dimension of this section is given by &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;d\theta&amp;lt;/math&amp;gt; which is the infinitesimal angular size. So, the infinitesimal charge contribution, &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;dQ&amp;lt;/math&amp;gt;, is&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; dQ = \frac{Q}{2\pi}d\theta &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Compute infinitesimal electric field contribution===&lt;br /&gt;
&lt;br /&gt;
Let us define some arbitrary location at which we are observing this ring of charge.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{r} = x\hat{x}+y\hat{y} + z\hat{z} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
in polar coordinates, we see this becomes&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{r} = Rcos(\theta)\hat{x} + Rsin(\theta)\hat{y} + z\hat{z} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Recall that both sine and cosine are periodic with the period of &amp;lt;math&amp;gt;2\pi &amp;lt;/math&amp;gt;. This will become important later.&lt;br /&gt;
&lt;br /&gt;
The magnitude of this vector is&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; |\vec{r}| = \sqrt{R^{2}+z^{2}} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
owing to the usage of the Pythagorean trigonometric identity.&lt;br /&gt;
&lt;br /&gt;
Now, we have what we need to write the electric field vector contributed by each piece of the ring of charge. Let this vector field piece be &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;d\vec{E}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; d\vec{E}=\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r}=\frac{1}{4\pi\epsilon_{0}}\frac{dQ}{(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Compute electric field vector===&lt;br /&gt;
&lt;br /&gt;
So, now all that is left is to sum everything up. We are summing over the circumference of a circle, so our path is defined by &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;0\leq\theta\leq 2\pi &amp;lt;/math&amp;gt;. Let us now set up our integral.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}=\int_{0}^{2\pi}\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} d\theta=\int_{0}^{2\pi}\frac{1}{4\pi\epsilon_{0}}\frac{Q}{2\pi(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z})d\theta&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Since both sine and cosine are &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;2\pi&amp;lt;/math&amp;gt; periodic functions, the &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;x&amp;lt;/math&amp;gt; and &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;y&amp;lt;/math&amp;gt; components of &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\vec{E}&amp;lt;/math&amp;gt; go to &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\vec{0}&amp;lt;/math&amp;gt;, which is very convenient. The result is&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \vec{E}=\frac{1}{4\pi\epsilon_{0}}\frac{Qz}{(z^{2}+R^{2})^{3/2}}\hat{z} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
===Remark===&lt;br /&gt;
&lt;br /&gt;
If the path we are interested in is over a half circle, third-circle or quarter-circle, or indeed any circular section, simply adjust the bounds of integration and the charge density to the ones required by the curve of interest.&lt;br /&gt;
&lt;br /&gt;
==Example Problems==&lt;br /&gt;
&lt;br /&gt;
===Easy===&lt;br /&gt;
&lt;br /&gt;
1.) Find the function &amp;lt;math&amp;gt;E(x)&amp;lt;/math&amp;gt; that represents the magnitude of the electric field along the center axis due to a uniformly charged ring of radius 0.04 m with total charge 8 C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We can use the derived formula for the electric field due to a charged ring. Only the horizontal components of the electric field will remain as the rest will cancel out.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;E(x) = \frac{1}{4\pi\epsilon_{0}}\frac{(8 C)*x}{((0.04 m)^2 + x^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
2.) A uniformly charged ring of radius 10.0 cm has a total charge of 91.0 µC. Find the electric field on the axis of the ring at the following distances from the center of the ring.&lt;br /&gt;
&lt;br /&gt;
a. 1 cm &lt;br /&gt;
&lt;br /&gt;
b. 5 cm &lt;br /&gt;
&lt;br /&gt;
c. 30 cm &lt;br /&gt;
&lt;br /&gt;
d. 100 cm&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Use the derived formula, and convert the given distances into meters and the charge into Coulombs. Plug these into &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;E(x) = \frac{1}{4\pi\epsilon_{0}}\frac{Q*x}{(x^2 + R^2)^\frac{3}{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
a. 8.069e6 N/C&lt;br /&gt;
&lt;br /&gt;
b. 29.3e6 N/C&lt;br /&gt;
&lt;br /&gt;
c. 7.76e6 N/C&lt;br /&gt;
&lt;br /&gt;
d. 8.06e5 N/C&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Find the electric field at a distance &amp;lt;math&amp;gt;z&amp;lt;/math&amp;gt; along the center axis away from a uniformly charged semicircular ring of radius R and total charge Q.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Solution&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We can tweak the same integral for a uniformly charged ring by changing the limits of integration.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E}=\int_{0}^{\pi}\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} d\theta=\int_{0}^{\pi}\frac{1}{4\pi\epsilon_{0}}\frac{Q}{\pi(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z})d\theta&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{E} = \frac{1}{4\pi\epsilon_{0}}\frac{Q}{\pi(R^{2}+z^{2})^{3/2}}(0\hat{x}+2R\hat{y}+{\pi}z\hat{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Added by AYESHA AHUJA SPRING 2020&lt;br /&gt;
&lt;br /&gt;
The first known time when charged rings were utilized to describe electromagnetism was during Faraday’s discovery of electrical induction. To conduct his experiments, Faraday used a ring made of iron that was attached to a battery. When this makeshift circuit was turned on it manipulated a compass needle by deflecting it. He showcased an induced current in the ring.&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
The idea of charge density is somewhat analogous to the idea of the mass density, which is useful in a variety of contexts, including the computation of the center of mass, the first and second moments of mass, which are useful in statics and rigid body dynamics. Instead of computing the uniform distribution of the mass of this ring, we are computing the uniform distribution of charge. This concept is also useful in visualizing what happens within a wire in a steady state circuit. The wire can be viewed to be a continuous length of rings of charge, which act as a channel through which electrons are transported, and that the electric field of these rings of charge pushes the electrons within the wire.&lt;br /&gt;
&lt;br /&gt;
It is also important in the context of Maxwell&#039;s equations, specifically in Gauss&#039;s Law and in the Maxwell-Faraday equation, which are concerned with electron flux and induced fields, respectively.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Charged Rod]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Disk]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Spherical Shell]]&lt;br /&gt;
&lt;br /&gt;
[[Charged Capacitor]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&amp;quot;Electric Field on the Axis of a Ring of Charge&amp;quot;.  University of Delaware Physics Library.  Adapted from Stephen Kevan&#039;s lecture on Electric Fields and Charge Distribution.  April 8, 1996.  http://www.physics.udel.edu/~watson/phys208/exercises/kevan/efield1.html&lt;br /&gt;
&lt;br /&gt;
Chabay, R., &amp;amp; Sherwood, B. (2015). Matter and Interactions (4th ed., Vol. 2, pp. 597-599). Wiley.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
All images produced by the author&lt;br /&gt;
&lt;br /&gt;
==External Links==&lt;br /&gt;
&lt;br /&gt;
https://www.youtube.com/watch?v=80mM3kSTZcE&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elelin.html&lt;br /&gt;
&lt;br /&gt;
http://www.physics.udel.edu/~watson/phys208/exercises/kevan/efield1.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Electric Fields]]&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24811</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24811"/>
		<updated>2016-11-27T16:46:31Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Mathematical Model===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png|370px|thumb|center|photo explaining conduction,convection,and radiation]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
== Examples ==&lt;br /&gt;
&lt;br /&gt;
=== Simple ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
=== Difficult ===&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|350px|alt=rudolf clausius|Photo of Rudolf Clausius]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24810</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24810"/>
		<updated>2016-11-27T16:46:03Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Mathematical Model===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png|370px|thumb|center|photo explaining conduction,convection,and radiation]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
== Examples ==&lt;br /&gt;
&lt;br /&gt;
=== Simple ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
=== Middle ===&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|350px|alt=rudolf clausius|Photo of Rudolf Clausius]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24809</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24809"/>
		<updated>2016-11-27T16:44:53Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Mathematical Model===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png|370px|thumb|center|photo explaining conduction,convection,and radiation]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|350px|alt=rudolf clausius|Photo of Rudolf Clausius]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24808</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24808"/>
		<updated>2016-11-27T16:34:17Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png|370px|thumb|center|photo explaining conduction,convection,and radiation]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|350px|alt=rudolf clausius|Photo of Rudolf Clausius]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24807</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24807"/>
		<updated>2016-11-27T16:34:00Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Thermal Energy and Temperature */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png|370px|thumb|center|photo explaining conduction,convection,and radiation]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|400px|alt=rudolf clausius|Photo of Rudolf Clausius]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24806</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24806"/>
		<updated>2016-11-27T16:32:51Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Thermal Energy and Temperature */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png|thumb|center|photo explaining conduction,convection,and radiation]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|400px|alt=rudolf clausius|Photo of Rudolf Clausius]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24805</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24805"/>
		<updated>2016-11-27T16:31:59Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|400px|alt=rudolf clausius|Photo of Rudolf Clausius]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24804</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24804"/>
		<updated>2016-11-27T16:31:43Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg||Rudolf Clausius ]]&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|400px|alt=rudolf clausius|Photo of Rudolf Clausius]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24803</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24803"/>
		<updated>2016-11-27T16:31:24Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg||Rudolf Clausius ]]&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb|center|400px|alt=rudolf clausius|Photo of Rudolf Clausius&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24802</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24802"/>
		<updated>2016-11-27T16:28:40Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg||Rudolf Clausius ]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24801</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24801"/>
		<updated>2016-11-27T16:28:21Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|  Rudolf Clausius ]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24800</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24800"/>
		<updated>2016-11-27T16:27:44Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
[[File:Rudolf_clausius.jpg|thumb]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24799</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24799"/>
		<updated>2016-11-27T16:23:50Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;br /&gt;
&lt;br /&gt;
http://teachers.oregon.k12.wi.us/mahr/assignments/thermal_energyvs_temp.pdf&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24798</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24798"/>
		<updated>2016-11-27T16:22:03Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Thermal Energy and Temperature */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
[[File:Heat_transfer_for_Heat_Conduction_2010-08-17.png]]&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24797</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24797"/>
		<updated>2016-11-27T16:16:57Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Heat Transfer */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, convection, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24755</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24755"/>
		<updated>2016-11-27T08:16:13Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24754</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24754"/>
		<updated>2016-11-27T08:15:44Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24753</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24753"/>
		<updated>2016-11-27T08:15:25Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24752</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24752"/>
		<updated>2016-11-27T08:15:10Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24751</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24751"/>
		<updated>2016-11-27T08:14:56Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = {27.576°C}&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24750</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24750"/>
		<updated>2016-11-27T08:12:32Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(43°C - 84°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {-2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((1.12kg)(5.16J/gc)(28°C) + ((.044kg)(2.2J/gc)(17°C))/((1.12)(5.16J/gc)+(.044)(2.2J/gc)) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24749</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24749"/>
		<updated>2016-11-27T08:09:16Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_f-T_it) + m_sc_s(T_f-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f} = { ((m_tc_tT_it) + (m_sc_sT_is))/(m_tc_t+m_sc_s) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24748</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24748"/>
		<updated>2016-11-27T08:08:28Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_ft-T_it) + m_sc_s(T_fs-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_f-m_tc_tT_it )+ (m_sc_sT_f-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{t_f(m_tc_t+m_sc_s)} = { (m_tc_tT_it) + (m_sc_sT_is) }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24747</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24747"/>
		<updated>2016-11-27T08:05:56Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_ft-T_it) + m_sc_s(T_fs-T_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {(m_tc_tT_ft-m_tc_tT_it )+ (m_sc_sT_fs-m_sc_sT_is)  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24746</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24746"/>
		<updated>2016-11-27T08:05:11Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tT_ft-T_it + m_sc_sT_fs-T_is  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tT_ft-m_tc_tT_it + m_sc_sT_fs-m_sc_sT_is  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24744</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24744"/>
		<updated>2016-11-27T07:56:15Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?(T is turkey, S is sauce)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tT_ft-T_it + m_sc_sT_fs-T_is  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24743</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24743"/>
		<updated>2016-11-27T07:55:45Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tT_ft-T_it + m_sc_sT_fs-T_is  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24742</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24742"/>
		<updated>2016-11-27T07:54:55Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tTf-T_i + m_sc_sTf-T_i  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24741</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24741"/>
		<updated>2016-11-27T07:54:40Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tTf-T_i + m_sc_sTf-T_i  }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24740</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24740"/>
		<updated>2016-11-27T07:54:09Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tTf-T_i + mc∆T }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24739</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24739"/>
		<updated>2016-11-27T07:53:44Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tT_f_t-T_i_t + mc∆T }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24738</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24738"/>
		<updated>2016-11-27T07:53:14Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_tT_(ft)-T_(it) + mc∆T }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24737</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24737"/>
		<updated>2016-11-27T07:52:44Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc_t(T_ft)-T_it + mc∆T }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24736</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24736"/>
		<updated>2016-11-27T07:52:09Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {m_tc∆T + mc∆T }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24735</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24735"/>
		<updated>2016-11-27T07:51:41Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆&#039;&#039;&#039;EthermalT&#039;&#039;&#039; + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {mc∆T + mc∆T }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24734</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24734"/>
		<updated>2016-11-27T07:51:14Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {[[∆EthermalT]] + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {[[mc∆T]] + mc∆T }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24733</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24733"/>
		<updated>2016-11-27T07:50:06Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esystem} = {∆EthermalT + ∆EthermalS }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24732</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24732"/>
		<updated>2016-11-27T07:49:19Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836 J}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24731</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24731"/>
		<updated>2016-11-27T07:49:01Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {2719.836}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24730</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24730"/>
		<updated>2016-11-27T07:47:35Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Thermal Energy and Temperature */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
=== Heat Transfer ===&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24729</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24729"/>
		<updated>2016-11-27T07:47:12Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Heat Transfer &amp;lt;/b&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
(1) On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
(2) You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24728</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24728"/>
		<updated>2016-11-27T07:46:47Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Thermal Energy and Temperature */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Heat Transfer &amp;lt;/b&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Temperature Change &amp;lt;/b&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24727</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24727"/>
		<updated>2016-11-27T07:46:01Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Temperature Change &amp;lt;/b&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24726</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24726"/>
		<updated>2016-11-27T07:45:35Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Temperature Change &amp;lt;/b&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system?&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24725</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24725"/>
		<updated>2016-11-27T07:44:39Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Temperature Change &amp;lt;/b&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system? &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;{∆Esys} = {∆EthermalT + ∆EthermalS} = 0&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24724</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24724"/>
		<updated>2016-11-27T07:43:50Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Temperature Change &amp;lt;/b&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system? &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;{∆Esys} = {∆EthermalT + ∆EthermalS} = 0&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esys} = {mc(Tf-Ti)+ mc(Tf-Ti)} = 0&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esys} = {∆EthermalT + ∆EthermalS} = 0&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Esys} = {∆EthermalT + ∆EthermalS} = 0&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24723</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Temperature&amp;diff=24723"/>
		<updated>2016-11-27T07:40:21Z</updated>

		<summary type="html">&lt;p&gt;Ayeshaahuja: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Written by Ju Yup Kim&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Edited/Claimed by Ayesha Ahuja&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Defining temperature==&lt;br /&gt;
&lt;br /&gt;
[[File:Tempfigure.gif|300px|thumb|right(position)|]]&lt;br /&gt;
Temperature is measure of average kinetic energy of the particles in a system. Difference between temperature and heat is that heat is the sum of all the kinetic energies of the particles in a system. Adding heat to a system causes its temperature to rise. Newton&#039;s zeroth law states that a system reaches a thermal equilibrium when there is no observable change in temperature between a system. Therefore, the change in temperature causes heat to flow from a high temperature system to a low temperature system. When systems with different temperature is in contact, molecules with higher kinetic energy collide with molecules with lower kinetic energy, kinetic energy is passed from the molecules with more kinetic energy to those with less kinetic energy. This molecular level of kinetic energy transfer will happen until average kinetic energy of the particles in each systems reach the average of two.&lt;br /&gt;
&lt;br /&gt;
 The relationship between heat transfer and temperature can be modeled with this equation:&lt;br /&gt;
 Q = m c Delta T&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Measurement===&lt;br /&gt;
[[File:Thermometer11.jpg|370px|thumb|right(position)|]]&lt;br /&gt;
A thermometer is a device used to measure temperature. It is placed in contact with an object and allowed to reach thermal equilibrium with the object. The operation of a thermometer is based on some property, such as volume, that varies with temperature. For example, mercury in a mercury thermometer expands to a degree depending on a temperature of the object and the level of the mercury in side the glass tube rises or descends.&lt;br /&gt;
Temperature can be measured in numbers by three temperature scales: Celsius, Fahrenheit, and Kelvin. Celsius scale sets freezing point of the water at zero and boiling point at 100, and Fahrenheit scale sets freezing point of the water at 32 degrees and boiling point of the water at 212 degrees. Kelvin scale is designed to go to zero at absolute zero, the minimum temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The relationship between temperature scales:&lt;br /&gt;
 &lt;br /&gt;
 (degrees)K = 273.15 + (degrees)C        (degrees)C = (5/9)*((degrees)F-32)        (degrees)F = (9/5)*(degrees)C+32&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Thermal Energy and Temperature==&lt;br /&gt;
The &#039;&#039;&#039;temperature&#039;&#039;&#039; and the &#039;&#039;&#039;thermal energy&#039;&#039;&#039; of an object are both measures of how much kinetic energy is acting on the particles of the material. However, thermal energy is the total kinetic energy of every single particle in the material. Temperature is the average speed of the particles in the material. When the temperature of an object is high the particles move fast and are further apart and when the temperature is low they move slower and closer together. When looking at an more than one object the total thermal energy transferred between two objects of different temperatures is referred to as &#039;&#039;&#039;heat&#039;&#039;&#039; ; generally the transfer is from a hotter to a colder temperature.  &lt;br /&gt;
&lt;br /&gt;
Heat transfers from objects of lower energy to objects of higher energy. There are three main types of heat transfer: conduction, conviction, and radiation. Conduction is seen as the transfer of energy from molecule to molecule. Convection is the energy transferred by the movement and motion of mass. Lastly, radiation is the the transfer of energy by waves.&lt;br /&gt;
&lt;br /&gt;
In physics, conduction is generally the type of heat transfer we focus on. By looking at the formula for thermal energy we can determine the change in energy of a system or the change in temperature of a system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Examples ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Temperature Change &amp;lt;/b&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
On thanksgiving morning your mom cooked a turkey with a mass of 12.55 kg and a temperature of 85°C coming out of the oven. By the time everyone is seated at the table and ready to eat the turkey is now 43°C. Determine the thermal energy of the turkey. The specific heat C for the Turkey is 5.16 J/(gC). &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of the turkey and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the turkey and &amp;lt;math&amp;gt;{∆T}&amp;lt;/math&amp;gt;  is the change in temperature of the turkey. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{∆Ethermal} = {(12.55kg)(5.16J/(gC))(85°C - 43°C) }&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
You take a slice of the turkey (mass: 1.12 kg) at 28°C and place some sauce on top. The sauce has a mass of .044 kg  and an initial temperature of 17°C , and a specific heat of 2.2 J/(gC). Looking at the turkey and sauce as a closed system what is the final temperature of the entire system? &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
EQ 1: &amp;lt;math&amp;gt;{∆Ethermal} = {mc∆T}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;{m}&amp;lt;/math&amp;gt; is the &#039;&#039;&#039;mass&#039;&#039;&#039; of an object and &amp;lt;math&amp;gt;{c}&amp;lt;/math&amp;gt; is the specific heat of the object and &amp;lt;math&amp;gt;{}&amp;lt;/math&amp;gt;  amount of work acting on the system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
EQ 2: &amp;lt;math&amp;gt;{∆Esys} = {∆E_thermalT} + ∆E_thermalS} = 0&lt;br /&gt;
&lt;br /&gt;
EQ 3: &amp;lt;math&amp;gt; E_{Rest}=mc^2 &amp;lt;/math&amp;gt; - Rest Energy, where &amp;lt;b&amp;gt;m&amp;lt;/b&amp;gt; is the mass and &amp;lt;b&amp;gt;c&amp;lt;/b&amp;gt; is the speed of light.&lt;br /&gt;
&lt;br /&gt;
EQ 4: &amp;lt;math&amp;gt;K=\frac{1}{2}mv²&amp;lt;/math&amp;gt; - Kinetic Energy, where &amp;lt;b&amp;gt;m&amp;lt;/b&amp;gt; is the mass and &amp;lt;b&amp;gt;v&amp;lt;/b&amp;gt; is the velocity (for speeds less than the speed of light).&lt;br /&gt;
&lt;br /&gt;
EQ 5: &amp;lt;math&amp;gt;∆E_{Thermal} = mC∆T &amp;lt;/math&amp;gt; - Thermal energy, were &amp;lt;b&amp;gt;m&amp;lt;/b&amp;gt; is the mass, &amp;lt;b&amp;gt;C&amp;lt;/b&amp;gt; is the specific heat of water (4.2 J/g/K), and &amp;lt;b&amp;gt;T&amp;lt;/b&amp;gt; is temperature.&lt;br /&gt;
&lt;br /&gt;
== Thermal Expansion ==&lt;br /&gt;
&lt;br /&gt;
Change in temperature through heat transfer can change the matter to change in shape, area, and volume. When a substance is heated, the kinetic energy of its molecules increases. Then the molecules begin moving more and average separation between molecules become larger, and thus volume of the substance changes. The degree of expansion divided by the change in temperature is called the material&#039;s coefficient of thermal expansion and generally varies with temperature and the object and state of matter of the object.&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!  Material  !! Fractional expansion per degree C x10^-6 !! Fractional expansion per degree F x10^-6&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, ordinary&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Glass, pyrex&lt;br /&gt;
| 4&lt;br /&gt;
| 2.2&lt;br /&gt;
|-&lt;br /&gt;
!  Quartz, fused&lt;br /&gt;
| .59&lt;br /&gt;
| .33&lt;br /&gt;
|-&lt;br /&gt;
!  Aluminum&lt;br /&gt;
| 24&lt;br /&gt;
| 13&lt;br /&gt;
|-&lt;br /&gt;
!  Brass&lt;br /&gt;
| 19&lt;br /&gt;
| 11&lt;br /&gt;
|-&lt;br /&gt;
!  Copper&lt;br /&gt;
| 17&lt;br /&gt;
| 9.4&lt;br /&gt;
|-&lt;br /&gt;
!  Iron&lt;br /&gt;
| 12&lt;br /&gt;
| 6.7&lt;br /&gt;
|-&lt;br /&gt;
!  Steel&lt;br /&gt;
| 13&lt;br /&gt;
| 7.2&lt;br /&gt;
|-&lt;br /&gt;
!  Platinum&lt;br /&gt;
| 9&lt;br /&gt;
| 5&lt;br /&gt;
|-&lt;br /&gt;
!  Tungsten&lt;br /&gt;
| 4.3&lt;br /&gt;
| 2.4&lt;br /&gt;
|-&lt;br /&gt;
!  Gold&lt;br /&gt;
| 14&lt;br /&gt;
| 7.8&lt;br /&gt;
|-&lt;br /&gt;
!  Silver&lt;br /&gt;
| 18&lt;br /&gt;
| 10&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
Early explanations of heat were thoroughly confused with explanations of combustion. J. J. Becher and George Ernst Stahl introduced the phlogiston theory of combustion in the 17th century, and phlogiston was thought to be the substance of heat.&lt;br /&gt;
&lt;br /&gt;
In late 18th century, Antoine Lavoisier argued that phlogiston theory is inconsistent and introduced Caloric theory. The suggested explanation was that when an object was heated, an invisible fluid called “caloric” was added to the object. Hot objects contained more caloric than cold objects. Caloric theory was popularly accepted until mid 19th century.&lt;br /&gt;
&lt;br /&gt;
Followed by introduction of  caloric theory, Count Rumford found that boring a cannon repeatedly does not result in heat producing ability, and therefore caloric is not lost. This proposed that caloric might not be a substance though the experimental ambiguity in his experiment were widely considered controversial.&lt;br /&gt;
&lt;br /&gt;
In mid 19th century, Rudolf Clausius showed that Rumford&#039;s argument and Caloric theory can be agreeable if the caloric theory include the principle of conservation of energy in place of its original principle of conservation of heat. By doing so, the caloric theory was able to be evolved into modern thermodynamics where heat may be put as a thermal energy which is equivalent to kinetic energy of some particles of the substance.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/tables/thexp.html&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/temper.html&lt;/div&gt;</summary>
		<author><name>Ayeshaahuja</name></author>
	</entry>
</feed>