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		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21504</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21504"/>
		<updated>2016-04-15T20:17:57Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C). Specific heat is important as it can determine the thermal interaction a material has with other materials and objects. Also, we can test the validity of models with specific heat since it is experimentally measurable.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat for sold can be calculated by the change in the energy of the atoms over the change in temperature. Change in the energy of the atom is calculated by change in the energy of the system divided by the number of atoms in the substance.&lt;br /&gt;
&lt;br /&gt;
The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039; The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
Einstein and Debye had developed models for specific heat separately with Einstien&#039;s model saying that low energy excitation of a solid material was caused by oscillation of a single atom, whereas Debye&#039;s model stated that phonons or collective modes iterating through the material caused the excitations. However, these two models are able to be extended together to find the specific heat given by the formula:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:einstein debye.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only volume or pressure is held constant at a time. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. In the formula below, the gas has a constant volume:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature. &lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://www.tutorvista.com/content/physics/physics-iii/heat-and-thermodynamics/dulong-and-petit-law.php&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
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Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21483</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21483"/>
		<updated>2016-04-15T19:53:31Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: /* Specific Heats of Gases */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C). Specific heat is important as it can determine the thermal interaction a material has with other materials and objects. Also, we can test the validity of models with specific heat since its is experimentally measurable.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat for sold can be calculated by the change in the energy of the atoms over the change in temperature. Change in the energy of the atom is calculated by Change in the energy of the system divided by the number of atoms in the substance.&lt;br /&gt;
&lt;br /&gt;
The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039;The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
Einstein and Debye had developed models for specific heat separately with Einstien&#039;s model saying that low energy excitation of a solid material was caused by oscillation of a single atom, whereas Debye&#039;s model stated that phonons or collective modes iterating through the material caused the excitations. However, these two models are able to be extended together to find the specific heat given by the formula:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:einstein debye.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only volume or pressure is held constant at a time. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. In the formula below, the gas has a constant volume:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature. &lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://www.tutorvista.com/content/physics/physics-iii/heat-and-thermodynamics/dulong-and-petit-law.php&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21482</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21482"/>
		<updated>2016-04-15T19:41:02Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C). Specific heat is important as it can determine the thermal interaction a material has with other materials and objects. Also, we can test the validity of models with specific heat since its is experimentally measurable.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat for sold can be calculated by the change in the energy of the atoms over the change in temperature. Change in the energy of the atom is calculated by Change in the energy of the system divided by the number of atoms in the substance.&lt;br /&gt;
&lt;br /&gt;
The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039;The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
Einstein and Debye had developed models for specific heat separately with Einstien&#039;s model saying that low energy excitation of a solid material was caused by oscillation of a single atom, whereas Debye&#039;s model stated that phonons or collective modes iterating through the material caused the excitations. However, these two models are able to be extended together to find the specific heat given by the formula:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:einstein debye.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://www.tutorvista.com/content/physics/physics-iii/heat-and-thermodynamics/dulong-and-petit-law.php&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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Main page&lt;br /&gt;
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This page has been accessed 525 times.&lt;br /&gt;
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Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21481</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21481"/>
		<updated>2016-04-15T19:39:52Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C). Specific heat is important as it can determine the thermal interaction a material has with other materials and objects. Also, we can test the validity of models with specific heat since its is experimentally measurable.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat for sold can be calculated by the change in the energy of the atoms over the change in temperature. Change in the energy of the atom is calculated by Change in the energy of the system divided by the number of atoms in the substance.&lt;br /&gt;
&lt;br /&gt;
The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039;The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
Einstein and Debye had developed models for specific heat separately with Einstien&#039;s model saying that low energy excitation of a solid material was caused by oscillation of a single atom, whereas Debye&#039;s model stated that phonons or collective modes iterating through the material caused the excitations. However, these two models are able to be extended together to find the specific heat given by the formula:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:einstein debye.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://www.tutorvista.com/content/physics/physics-iii/heat-and-thermodynamics/dulong-and-petit-law.php&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21480</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21480"/>
		<updated>2016-04-15T19:38:43Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:Example.jpg]]&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C). Specific heat is important as it can determine the thermal interaction a material has with other materials and objects. Also, we can test the validity of models with specific heat since its is experimentally measurable.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat for sold can be calculated by the change in the energy of the atoms over the change in temperature. Change in the energy of the atom is calculated by Change in the energy of the system divided by the number of atoms in the substance.&lt;br /&gt;
&lt;br /&gt;
The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039;The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
Einstein and Debye had developed models for specific heat separately with Einstien&#039;s model saying that low energy excitation of a solid material was caused by oscillation of a single atom, whereas Debye&#039;s model stated that phonons or collective modes iterating through the material caused the excitations. However, these two models are able to be extended together to find the specific heat given by the formula:&lt;br /&gt;
&lt;br /&gt;
[[File:einstein debye.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://www.tutorvista.com/content/physics/physics-iii/heat-and-thermodynamics/dulong-and-petit-law.php&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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Main page&lt;br /&gt;
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		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Einstein_debye.png&amp;diff=21479</id>
		<title>File:Einstein debye.png</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Einstein_debye.png&amp;diff=21479"/>
		<updated>2016-04-15T19:37:14Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: Rbaker72 uploaded a new version of &amp;amp;quot;File:Einstein debye.png&amp;amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
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	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Einstein_debye.png&amp;diff=21478</id>
		<title>File:Einstein debye.png</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Einstein_debye.png&amp;diff=21478"/>
		<updated>2016-04-15T19:36:08Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
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	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21477</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21477"/>
		<updated>2016-04-15T19:35:36Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C). Specific heat is important as it can determine the thermal interaction a material has with other materials and objects. Also, we can test the validity of models with specific heat since its is experimentally measurable.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat for sold can be calculated by the change in the energy of the atoms over the change in temperature. Change in the energy of the atom is calculated by Change in the energy of the system divided by the number of atoms in the substance.&lt;br /&gt;
&lt;br /&gt;
The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039;The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
Einstein and Debye had developed models for specific heat separately with Einstien&#039;s model saying that low energy excitation of a solid material was caused by oscillation of a single atom, whereas Debye&#039;s model stated that phonons or collective modes iterating through the material caused the excitations. However, these two models are able to be extended together to find the specific heat given by the formula:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:einstein debye.png|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://www.tutorvista.com/content/physics/physics-iii/heat-and-thermodynamics/dulong-and-petit-law.php&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
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		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21474</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21474"/>
		<updated>2016-04-15T18:20:45Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C). Specific heat is important as it can determine the thermal interaction a material has with other materials and objects. Also, we can test the validity of models with specific heat since its is experimentally measurable.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat for sold can be calculated by the change in the energy of the atoms over the change in temperature. Change in the energy of the atom is calculated by Change in the energy of the system divided by the number of atoms in the substance.&lt;br /&gt;
&lt;br /&gt;
The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039;The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://www.tutorvista.com/content/physics/physics-iii/heat-and-thermodynamics/dulong-and-petit-law.php&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Main page&lt;br /&gt;
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Random page&lt;br /&gt;
Help&lt;br /&gt;
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&lt;br /&gt;
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Printable version&lt;br /&gt;
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&lt;br /&gt;
This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
This page has been accessed 525 times.&lt;br /&gt;
Privacy policy&lt;br /&gt;
About Physics Book&lt;br /&gt;
Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21473</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21473"/>
		<updated>2016-04-15T18:03:34Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat for sold can be calculated by the change in the energy of the atoms over the change in temperature. Change in the energy of the atom is calculated by Change in the energy of the system divided by the number of atoms in the substance.&lt;br /&gt;
&lt;br /&gt;
The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039;The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://www.tutorvista.com/content/physics/physics-iii/heat-and-thermodynamics/dulong-and-petit-law.php&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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Main page&lt;br /&gt;
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This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
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Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21467</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21467"/>
		<updated>2016-04-15T17:35:03Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
In 1819, French physicists, Pierre Louis Dulong and Alexis Thérèse Petit, discovered that the average molar specific heat for metals are approximately the same and equal to 25 J mole-1 oC-1 or roughly 3R where R is the gas constant for one mole. In this law, the amount of heat required to change the temperature is dependent on the number of molecules in the substance and not the mass.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Example&#039;&#039;&#039;The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Main page&lt;br /&gt;
Recent changes&lt;br /&gt;
Random page&lt;br /&gt;
Help&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Tools&lt;br /&gt;
&lt;br /&gt;
What links here&lt;br /&gt;
Related changes&lt;br /&gt;
Upload file&lt;br /&gt;
Special pages&lt;br /&gt;
Printable version&lt;br /&gt;
Permanent link&lt;br /&gt;
Page information&lt;br /&gt;
&lt;br /&gt;
This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
This page has been accessed 525 times.&lt;br /&gt;
Privacy policy&lt;br /&gt;
About Physics Book&lt;br /&gt;
Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21458</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21458"/>
		<updated>2016-04-15T16:57:04Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
This law deals with substances when the are at room temperature. &lt;br /&gt;
&lt;br /&gt;
The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Main page&lt;br /&gt;
Recent changes&lt;br /&gt;
Random page&lt;br /&gt;
Help&lt;br /&gt;
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This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
This page has been accessed 525 times.&lt;br /&gt;
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Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21456</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21456"/>
		<updated>2016-04-15T16:51:08Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. These are the Dulong-Petit Law and the Einstein-Deybe model. The molar specific heats of most solids at room temperature are practically constant, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. This behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/dulong.html#c1&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/debye.html#c2&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Main page&lt;br /&gt;
Recent changes&lt;br /&gt;
Random page&lt;br /&gt;
Help&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Tools&lt;br /&gt;
&lt;br /&gt;
What links here&lt;br /&gt;
Related changes&lt;br /&gt;
Upload file&lt;br /&gt;
Special pages&lt;br /&gt;
Printable version&lt;br /&gt;
Permanent link&lt;br /&gt;
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&lt;br /&gt;
This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
This page has been accessed 525 times.&lt;br /&gt;
Privacy policy&lt;br /&gt;
About Physics Book&lt;br /&gt;
Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21454</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21454"/>
		<updated>2016-04-15T16:46:53Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. The molar specific heats of most solids at room temperature are almost the same, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. The lower temperature behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/spht.html&lt;br /&gt;
http://scienceworld.wolfram.com/physics/SpecificHeat.html&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/dulong.html#c1&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/debye.html#c2&lt;br /&gt;
Matter &amp;amp; Interactions Vol I. Chabay Sherwood&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Main page&lt;br /&gt;
Recent changes&lt;br /&gt;
Random page&lt;br /&gt;
Help&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Tools&lt;br /&gt;
&lt;br /&gt;
What links here&lt;br /&gt;
Related changes&lt;br /&gt;
Upload file&lt;br /&gt;
Special pages&lt;br /&gt;
Printable version&lt;br /&gt;
Permanent link&lt;br /&gt;
Page information&lt;br /&gt;
&lt;br /&gt;
This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
This page has been accessed 525 times.&lt;br /&gt;
Privacy policy&lt;br /&gt;
About Physics Book&lt;br /&gt;
Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21453</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21453"/>
		<updated>2016-04-15T16:43:24Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
There are two ways to determine the specific heats of substances at the atomic level. The molar specific heats of most solids at room temperature are almost the same, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. The lower temperature behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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Main page&lt;br /&gt;
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Printable version&lt;br /&gt;
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&lt;br /&gt;
This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
This page has been accessed 525 times.&lt;br /&gt;
Privacy policy&lt;br /&gt;
About Physics Book&lt;br /&gt;
Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21450</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21450"/>
		<updated>2016-04-15T16:20:49Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. Since the specific heat of water is so high, water can be used for temperature regulation. Due to the difference in their atomic structures, the specific heat per gram for water is much higher than that for a metal. It is possible to predict the specific heat of an material, if you know about its atomic structure, as a rise in temperature is the increase in energy at the atomic level of substances. Generally, it is more more useful to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
The molar specific heats of most solids at room temperature are almost the same, which agrees with the Law of Dulong and Petit. At lower temperatures, the specific heats drop as atomic processes become more relevant. The lower temperature behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Main page&lt;br /&gt;
Recent changes&lt;br /&gt;
Random page&lt;br /&gt;
Help&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Tools&lt;br /&gt;
&lt;br /&gt;
What links here&lt;br /&gt;
Related changes&lt;br /&gt;
Upload file&lt;br /&gt;
Special pages&lt;br /&gt;
Printable version&lt;br /&gt;
Permanent link&lt;br /&gt;
Page information&lt;br /&gt;
&lt;br /&gt;
This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
This page has been accessed 525 times.&lt;br /&gt;
Privacy policy&lt;br /&gt;
About Physics Book&lt;br /&gt;
Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21449</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21449"/>
		<updated>2016-04-15T16:02:13Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use the formula;&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. The specific heat per gram for water is much higher than that for a metal. Therefore, there are two separate ways to calculate specific heats. Traditionally, it is more acceptable to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
The molar specific heats of most solids at room temperature are almost the same, which agrees with the Law of Dulong and Petit. At lower temperatures the specific heats drop as atomic processes become more relevant. The lower temperature behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
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		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Specific_heat_formula.png&amp;diff=21448</id>
		<title>File:Specific heat formula.png</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Specific_heat_formula.png&amp;diff=21448"/>
		<updated>2016-04-15T15:59:49Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21447</id>
		<title>Specific Heat</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Specific_Heat&amp;diff=21447"/>
		<updated>2016-04-15T15:59:11Z</updated>

		<summary type="html">&lt;p&gt;Rbaker72: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
Specific Heat, also known as the specific heat capacity, is defined as the amount of heat required to raise the temperature of a unit mass by one degree Celsius. The units for specific heat are Joules per gram-degree Celsius (J / g °C).&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The most common definition is that specific heat is the amount of heat needed to raise the temperature of a mass by 1 degree. The relationship between heat and temperature change is best defined by constant &amp;quot;C&amp;quot; in the equation &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Specific Heat Equation.gif]]&lt;br /&gt;
 &lt;br /&gt;
To calcuate specfic heat, use&lt;br /&gt;
&lt;br /&gt;
[[File:specific heat formula.png]]&lt;br /&gt;
&lt;br /&gt;
where the mass is in grams.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The relationship does not apply if a phase change is occurs because the heat added or removed during a phase change does not necessarily change the temperature. The specific heat most commonly known is the specific heat for water, which is 4.186 joule/gram °C or  1 calorie/gram °C. Water has a very large specific heat on a per-gram basis which means that it is very difficult to cause a change in its temperature. The specific heat per gram for water is much higher than that for a metal. Therefore, there are two separate ways to calculate specific heats. Traditionally, it is more acceptable to compare specific heats on a molecular level. &lt;br /&gt;
&lt;br /&gt;
The molar specific heats of most solids at room temperature are almost the same, which agrees with the Law of Dulong and Petit. At lower temperatures the specific heats drop as atomic processes become more relevant. The lower temperature behavior is  explained by the Einstein-Debye model of specific heat.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Law of Dulong and Petit ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The specific heat of copper is 0.386 Joules/gram degrees Celsius while the specific heat of Aluminum is 0.900 Joules/gram Celsius. Why is there such a difference? Specific heat is measured in Energy per unit mass, but it should be measured in Energy per mole for more similar specific heats for solids. The similar molar specific heats for solid metals are what define the Law of Dulong and Petit.&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong.gif]]     &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 The specific heats of metals, therefore should all be around 24.94 J/mol degrees Celsius. The specific heat at constant volume should be just the temperature derivative of that energy.&lt;br /&gt;
&lt;br /&gt;
Copper     0.386 J/gm K x 63.6 gm/mol = 24.6 J/mol K&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aluminum   0.900 J/gm K x 26.98 gm/ mol = 24.3 J/mol K &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Einstein Debye Model ==&lt;br /&gt;
[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For low temperatures, Einstein and Debye found that the Law of Dulong and Petit was not applicable. At lower temperatures, it was found that atomic interactions were deemed significant in calculating the  molar specific heat of an object. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File: Einstein Debye Graphs.gif]]&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
According to the Einstein Debye Model for Copper and Aluminum, two solid metals, specific heat varies much at lower temperatures and goes much below the Dulong-Petit Model. This is due to increased effects on specific heat by interatomic forces. However, for very high temperature values, the Einstein-Debye Model cannot be used. In fact, at high temperatures, Einstein&#039;s expression of specific heat, reduces to the Dulong-Petit mathematical expression.&lt;br /&gt;
&lt;br /&gt;
Here is the Einstein Debye Equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye Equation.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For high Temperatures it may be reduced like this:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Einstein Debye for High Temperatures.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This actually reduces to the Dulong-Petit Formula for Specific Heat:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Dulong Petit.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Specific Heats of Gases===&lt;br /&gt;
&lt;br /&gt;
Specific heats of gases are generally expressed in their molar form due to the undefined volume or pressure of a gas. Usually only one is held constant. The first law of Thermodynamics helps to derive the formulas for specific heat for constant pressure and the specific heat for constant volume. Here is the equation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:first law.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There are two specific heats for gases, one for gases at a constant volume and one gases at a constant pressure. Since delta V is constant, or a constant volume the equation is:&lt;br /&gt;
&lt;br /&gt;
[[File:constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an ideal monatomic gas the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant volume.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a constant pressure, specific heat can be derived as:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Constant Pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For and ideal monatomic gas, the molar specific heat should be around:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ideal for constant pressure.gif]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where Q is heat, n is number of moles, and delta T is change in Temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The molar specific heats of gases all gravitate towards these ranges depending on the conditions the gas is kept in.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
# Specific heat can have a lot to do with prosthetic manufacturing, which is huge in Biomedical Engineering. Prosthetics materials must be durable and easy to manipulate in a normal range of temperatures. In order to created medical devices, specific heats must be known, especially for welding or molding things, which require a specific temperature to be effective. At higher temperatures, the Dulong-Petit law must be used to calculate the specific heat of an object. Especially for solid metal objects, which would be used in prosthetics, Dulong-Petit is especially useful.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Heat Capacity&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.wisegeek.org/what-is-specific-heat.htm]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/emcon.html#emcon&lt;br /&gt;
&lt;br /&gt;
[[Properties of Matter]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Claimed by Felix Joseph&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
Main page&lt;br /&gt;
Recent changes&lt;br /&gt;
Random page&lt;br /&gt;
Help&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Tools&lt;br /&gt;
&lt;br /&gt;
What links here&lt;br /&gt;
Related changes&lt;br /&gt;
Upload file&lt;br /&gt;
Special pages&lt;br /&gt;
Printable version&lt;br /&gt;
Permanent link&lt;br /&gt;
Page information&lt;br /&gt;
&lt;br /&gt;
This page was last modified on 29 November 2015, at 23:04.&lt;br /&gt;
This page has been accessed 525 times.&lt;br /&gt;
Privacy policy&lt;br /&gt;
About Physics Book&lt;br /&gt;
Disclaimers&lt;/div&gt;</summary>
		<author><name>Rbaker72</name></author>
	</entry>
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