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	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=19034</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=19034"/>
		<updated>2015-12-06T03:24:55Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
[[File:Io15.gif|200px|thumb|right|alt text]]&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has to have coils much larger than the radius. The length of the coil is much larger than the diameter, and its often wrapped around a metal rod. The rod produces a magnetic field when an electric current is passed through it. &lt;br /&gt;
&lt;br /&gt;
A solenoid is a type of electromagnet when it is used to create a controlled magnetic field or if it is used to resist a current changing, then it is an inductor. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
&lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(-L/2, L/2+dx, dx):&lt;br /&gt;
&lt;br /&gt;
     for y in [-.05,-.04, -.02,-.01,0,.01,.02,.03,.04,.05]:&lt;br /&gt;
&lt;br /&gt;
          aa = arrow (pos = (x,y,zz), axis = (0,0,0), color = color.cyan, shaftwidth = .0003)&lt;br /&gt;
&lt;br /&gt;
          Barrows.append(aa)&lt;br /&gt;
&lt;br /&gt;
for b in Barrows:&lt;br /&gt;
&lt;br /&gt;
     for point in solenoid.pos:&lt;br /&gt;
&lt;br /&gt;
          dl = point - dlstart&lt;br /&gt;
&lt;br /&gt;
          r = b.pos - (dlstart +dl/2)&lt;br /&gt;
&lt;br /&gt;
          b.axis = b.axis + (-bscale*kmag*I*cross(dl, norm(r)))/mag(r)**2&lt;br /&gt;
&lt;br /&gt;
          dlstart = point&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula, shown as the top image on the right.  &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|Equation]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2, shown as the bottom image on the right. &lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|The Integral]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|Andre-Marie Ampere]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf&lt;br /&gt;
http://www.deltrol-controls.com/products/solenoids&lt;br /&gt;
https://www.pa.msu.edu/courses/2000fall/PHY232/lectures/ampereslaw/solenoid.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18975</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18975"/>
		<updated>2015-12-06T03:20:34Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: /* External links */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
[[File:Io15.gif|200px|thumb|right|alt text]]&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. The length of the coil is much larger than the diameter, and its often wrapped around a metal rod. The rod produces a magnetic field when an electric current is passed through it. &lt;br /&gt;
&lt;br /&gt;
A solenoid is a type of electromagnet when it is used to create a controlled magnetic field or if it is used to resist a current changing, then it is an inductor. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
&lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(-L/2, L/2+dx, dx):&lt;br /&gt;
&lt;br /&gt;
     for y in [-.05,-.04, -.02,-.01,0,.01,.02,.03,.04,.05]:&lt;br /&gt;
&lt;br /&gt;
          aa = arrow (pos = (x,y,zz), axis = (0,0,0), color = color.cyan, shaftwidth = .0003)&lt;br /&gt;
&lt;br /&gt;
          Barrows.append(aa)&lt;br /&gt;
&lt;br /&gt;
for b in Barrows:&lt;br /&gt;
&lt;br /&gt;
     for point in solenoid.pos:&lt;br /&gt;
&lt;br /&gt;
          dl = point - dlstart&lt;br /&gt;
&lt;br /&gt;
          r = b.pos - (dlstart +dl/2)&lt;br /&gt;
&lt;br /&gt;
          b.axis = b.axis + (-bscale*kmag*I*cross(dl, norm(r)))/mag(r)**2&lt;br /&gt;
&lt;br /&gt;
          dlstart = point&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula, shown as the top image on the right.  &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|Equation]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2, shown as the bottom image on the right. &lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|The Integral]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|Andre-Marie Ampere]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf&lt;br /&gt;
http://www.deltrol-controls.com/products/solenoids&lt;br /&gt;
https://www.pa.msu.edu/courses/2000fall/PHY232/lectures/ampereslaw/solenoid.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18957</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18957"/>
		<updated>2015-12-06T03:19:40Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: /* External links */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
[[File:Io15.gif|200px|thumb|right|alt text]]&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. The length of the coil is much larger than the diameter, and its often wrapped around a metal rod. The rod produces a magnetic field when an electric current is passed through it. &lt;br /&gt;
&lt;br /&gt;
A solenoid is a type of electromagnet when it is used to create a controlled magnetic field or if it is used to resist a current changing, then it is an inductor. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
&lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(-L/2, L/2+dx, dx):&lt;br /&gt;
&lt;br /&gt;
     for y in [-.05,-.04, -.02,-.01,0,.01,.02,.03,.04,.05]:&lt;br /&gt;
&lt;br /&gt;
          aa = arrow (pos = (x,y,zz), axis = (0,0,0), color = color.cyan, shaftwidth = .0003)&lt;br /&gt;
&lt;br /&gt;
          Barrows.append(aa)&lt;br /&gt;
&lt;br /&gt;
for b in Barrows:&lt;br /&gt;
&lt;br /&gt;
     for point in solenoid.pos:&lt;br /&gt;
&lt;br /&gt;
          dl = point - dlstart&lt;br /&gt;
&lt;br /&gt;
          r = b.pos - (dlstart +dl/2)&lt;br /&gt;
&lt;br /&gt;
          b.axis = b.axis + (-bscale*kmag*I*cross(dl, norm(r)))/mag(r)**2&lt;br /&gt;
&lt;br /&gt;
          dlstart = point&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula, shown as the top image on the right.  &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|Equation]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2, shown as the bottom image on the right. &lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|The Integral]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|Andre-Marie Ampere]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18952</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18952"/>
		<updated>2015-12-06T03:19:25Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
[[File:Io15.gif|200px|thumb|right|alt text]]&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. The length of the coil is much larger than the diameter, and its often wrapped around a metal rod. The rod produces a magnetic field when an electric current is passed through it. &lt;br /&gt;
&lt;br /&gt;
A solenoid is a type of electromagnet when it is used to create a controlled magnetic field or if it is used to resist a current changing, then it is an inductor. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
&lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(-L/2, L/2+dx, dx):&lt;br /&gt;
&lt;br /&gt;
     for y in [-.05,-.04, -.02,-.01,0,.01,.02,.03,.04,.05]:&lt;br /&gt;
&lt;br /&gt;
          aa = arrow (pos = (x,y,zz), axis = (0,0,0), color = color.cyan, shaftwidth = .0003)&lt;br /&gt;
&lt;br /&gt;
          Barrows.append(aa)&lt;br /&gt;
&lt;br /&gt;
for b in Barrows:&lt;br /&gt;
&lt;br /&gt;
     for point in solenoid.pos:&lt;br /&gt;
&lt;br /&gt;
          dl = point - dlstart&lt;br /&gt;
&lt;br /&gt;
          r = b.pos - (dlstart +dl/2)&lt;br /&gt;
&lt;br /&gt;
          b.axis = b.axis + (-bscale*kmag*I*cross(dl, norm(r)))/mag(r)**2&lt;br /&gt;
&lt;br /&gt;
          dlstart = point&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula, shown as the top image on the right.  &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|Equation]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2, shown as the bottom image on the right. &lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|The Integral]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|Andre-Marie Ampere]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18901</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18901"/>
		<updated>2015-12-06T03:15:25Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
[[File:Io15.gif|200px|thumb|right|alt text]]&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. The length of the coil is much larger than the diameter, and its often wrapped around a metal rod. The rod produces a magnetic field when an electric current is passed through it. &lt;br /&gt;
&lt;br /&gt;
A solenoid is a type of electromagnet when it is used to create a controlled magnetic field or if it is used to resist a current changing, then it is an inductor. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
&lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(-L/2, L/2+dx, dx):&lt;br /&gt;
&lt;br /&gt;
     for y in [-.05,-.04, -.02,-.01,0,.01,.02,.03,.04,.05]:&lt;br /&gt;
&lt;br /&gt;
          aa = arrow (pos = (x,y,zz), axis = (0,0,0), color = color.cyan, shaftwidth = .0003)&lt;br /&gt;
&lt;br /&gt;
          Barrows.append(aa)&lt;br /&gt;
&lt;br /&gt;
for b in Barrows:&lt;br /&gt;
&lt;br /&gt;
     for point in solenoid.pos:&lt;br /&gt;
&lt;br /&gt;
          dl = point - dlstart&lt;br /&gt;
&lt;br /&gt;
          r = b.pos - (dlstart +dl/2)&lt;br /&gt;
&lt;br /&gt;
          b.axis = b.axis + (-bscale*kmag*I*cross(dl, norm(r)))/mag(r)**2&lt;br /&gt;
&lt;br /&gt;
          dlstart = point&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula, shown as the top image on the right.  &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|Equation]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2, shown as the bottom image on the right. &lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|The Integral]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|alt text]]&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18896</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18896"/>
		<updated>2015-12-06T03:15:02Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
[[File:Io15.gif|200px|thumb|right|alt text]]&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. The length of the coil is much larger than the diameter, and its often wrapped around a metal rod. The rod produces a magnetic field when an electric current is passed through it. &lt;br /&gt;
&lt;br /&gt;
A solenoid is a type of electromagnet when it is used to create a controlled magnetic field or if it is used to resist a current changing, then it is an inductor. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(-L/2, L/2+dx, dx):&lt;br /&gt;
&lt;br /&gt;
     for y in [-.05,-.04, -.02,-.01,0,.01,.02,.03,.04,.05]:&lt;br /&gt;
&lt;br /&gt;
          aa = arrow (pos = (x,y,zz), axis = (0,0,0), color = color.cyan, shaftwidth = .0003)&lt;br /&gt;
&lt;br /&gt;
          Barrows.append(aa)&lt;br /&gt;
&lt;br /&gt;
for b in Barrows:&lt;br /&gt;
&lt;br /&gt;
     for point in solenoid.pos:&lt;br /&gt;
&lt;br /&gt;
          dl = point - dlstart&lt;br /&gt;
&lt;br /&gt;
          r = b.pos - (dlstart +dl/2)&lt;br /&gt;
&lt;br /&gt;
          b.axis = b.axis + (-bscale*kmag*I*cross(dl, norm(r)))/mag(r)**2&lt;br /&gt;
&lt;br /&gt;
          dlstart = point&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula, shown as the top image on the right.  &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|Equation]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2, shown as the bottom image on the right. &lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|The Integral]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|alt text]]&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18708</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18708"/>
		<updated>2015-12-06T02:57:32Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
[[File:Io15.gif|200px|thumb|right|alt text]]]&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula, shown as the top image on the right.  &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|Equation]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2, shown as the bottom image on the right. &lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|The Integral]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|alt text]]&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Io15.gif&amp;diff=18697</id>
		<title>File:Io15.gif</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Io15.gif&amp;diff=18697"/>
		<updated>2015-12-06T02:56:54Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18676</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18676"/>
		<updated>2015-12-06T02:55:45Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula, shown as the top image on the right.  &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|Equation]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2, shown as the bottom image on the right. &lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|The Integral]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|alt text]]&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18660</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18660"/>
		<updated>2015-12-06T02:54:40Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula: &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg|200px|thumb|right|alt text]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2:&lt;br /&gt;
[[File:FullSizeRenderRads1.jpg|200px|thumb|right|alt text]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg|200px|thumb|right|alt text]]&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18648</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18648"/>
		<updated>2015-12-06T02:52:50Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoid so the number of loops in the length &amp;lt;math&amp;gt;\Delta x&amp;lt;/math&amp;gt; is N/L*&amp;lt;math&amp;gt;\Delta E&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
So this the equation we have so far using the magnetic field formula: &lt;br /&gt;
[[File:FullSizeRenderRadz.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Add Up all the Pieces &lt;br /&gt;
&lt;br /&gt;
The net magnetic field lies along the axis and the sum is &amp;lt;math&amp;gt;\Delta B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This can be turned into a integral from -L/2 to L/2:&lt;br /&gt;
[[File:FullSizeRenderRads1.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The integral can be solved out using a standard table of integrals or an integration calculator. &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg]]&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:FullSizeRenderRadz.jpg&amp;diff=18644</id>
		<title>File:FullSizeRenderRadz.jpg</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:FullSizeRenderRadz.jpg&amp;diff=18644"/>
		<updated>2015-12-06T02:52:15Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:FullSizeRenderRads1.jpg&amp;diff=18635</id>
		<title>File:FullSizeRenderRads1.jpg</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:FullSizeRenderRads1.jpg&amp;diff=18635"/>
		<updated>2015-12-06T02:51:32Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18579</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=18579"/>
		<updated>2015-12-06T02:44:26Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a solenoid, we need to do a three step process. &lt;br /&gt;
&lt;br /&gt;
Imagine a solenoid with a length L that is made up of N loops wound, each with a radius R and a current I. Each loop is one piece. &lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Due to One Piece &lt;br /&gt;
&lt;br /&gt;
The origin of the solenoid is at its center. To find the location of one piece we have to find the integration variable, which is x, and then the distance from the loop to the observation location is d-z. There are also N/L loops in the solenoud so the number of loops in the length &amp;lt;math&amp;gt;/Delta{x}&amp;lt;/math&amp;gt; is  &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
There are many applications to solenoids that we use as a part of our everyday lives. They can be found in medical equipment, air conditioning devices, electric locking mechanisms, cars, and many others. To find out more about each of these applications in detail please go to [[Solenoid Applications]]. &lt;br /&gt;
One example is the car starter solenoid. The starter solenoid receives a large electric current from the car battery and a small electric current from the ignition switch. When the switch is turned on, the small current forces the starter solenoid to close contacts and relays the large electric current to the starter motor. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg]]&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
Matters and Interactions, 3rd Edition&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=16582</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=16582"/>
		<updated>2015-12-05T23:13:54Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a sol&lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
[[File:Andre-marie-ampere-3.jpg]]&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Andre-marie-ampere-3.jpg&amp;diff=16576</id>
		<title>File:Andre-marie-ampere-3.jpg</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Andre-marie-ampere-3.jpg&amp;diff=16576"/>
		<updated>2015-12-05T23:13:37Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=16560</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=16560"/>
		<updated>2015-12-05T23:12:08Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a sol&lt;br /&gt;
[[File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Screen_Shot_2015-12-05_at_6.12.26_PM.jpg&amp;diff=16553</id>
		<title>File:Screen Shot 2015-12-05 at 6.12.26 PM.jpg</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Screen_Shot_2015-12-05_at_6.12.26_PM.jpg&amp;diff=16553"/>
		<updated>2015-12-05T23:11:27Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Solenoid1.jpg&amp;diff=16532</id>
		<title>File:Solenoid1.jpg</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Solenoid1.jpg&amp;diff=16532"/>
		<updated>2015-12-05T23:07:21Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=16488</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=16488"/>
		<updated>2015-12-05T23:01:18Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
To solve for the magnetic field of a sol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14454</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14454"/>
		<updated>2015-12-05T17:40:41Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of A Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14453</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14453"/>
		<updated>2015-12-05T17:40:11Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Andre-Marie Ampere originally coined the word &amp;quot;Solenoid&amp;quot; in the 1820&#039;s, which he used to describe a helical coil. He probably used solenoid while he was developing the theory for Ampere&#039;s Law, which can be used to find the magnetic field of a solenoid.&lt;br /&gt;
 &lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
[[Right-Hand Rule]]&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
[[Magnetic Field of Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.gouldvalve.com/wp-content/uploads/2009/05/typical-uses-pages-1-3.pdf]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html&lt;br /&gt;
http://www.bachofen.ch/fr/schalttechnik/ProdukteF_Composants/Befehlsgeraete_Schalter_Mikroschalter/Johnson_Electric_LEDEX_Solenoids_EN_2014.pdf&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category: Fields]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14410</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14410"/>
		<updated>2015-12-05T17:32:44Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14400</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14400"/>
		<updated>2015-12-05T17:29:51Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
.## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
.## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14384</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14384"/>
		<updated>2015-12-05T17:24:26Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
A solenoid has a length of .5 meters and a radius of .03 meters and wound around 50 times a wire that has a current of 1 ampere. Find the magnetic field vectors. &lt;br /&gt;
from visual import ∗&lt;br /&gt;
&lt;br /&gt;
scene . width=1024 scene.x = scene.y = 0&lt;br /&gt;
&lt;br /&gt;
scene . background = color . white&lt;br /&gt;
&lt;br /&gt;
L = 0.5&lt;br /&gt;
&lt;br /&gt;
R = 0.03&lt;br /&gt;
&lt;br /&gt;
kmag = 1e-7&lt;br /&gt;
&lt;br /&gt;
I = 1&lt;br /&gt;
&lt;br /&gt;
Nturns=50. ## number of turns in solenoid&lt;br /&gt;
&lt;br /&gt;
Nelts=20. ## number of line segments per turn&lt;br /&gt;
&lt;br /&gt;
bscale = 600. ## scale factor for B arrows&lt;br /&gt;
&lt;br /&gt;
## make a solenoid&lt;br /&gt;
&lt;br /&gt;
dxx = L/(Nturns∗Nelts)&lt;br /&gt;
&lt;br /&gt;
xx = arange(L/2., L/2+dxx, dxx)&lt;br /&gt;
&lt;br /&gt;
omega = 2∗pi∗Nturns/L&lt;br /&gt;
&lt;br /&gt;
solenoid = curve(x=xx, y=R∗sin(xx∗omega), z=R∗cos(xx∗omega), color=(.9,.7,0),radius =0.001)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
## make a list of zero lth arrows at observation locations &lt;br /&gt;
&lt;br /&gt;
Barrows =[] ## empty list&lt;br /&gt;
&lt;br /&gt;
dx = L/4.&lt;br /&gt;
&lt;br /&gt;
zz=0.&lt;br /&gt;
&lt;br /&gt;
for x in arange(&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14357</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14357"/>
		<updated>2015-12-05T17:17:47Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the &amp;lt;math&amp;gt;\Delta \vec{B}&amp;lt;/math&amp;gt;,&lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
(picture)&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable &amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt;, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
&lt;br /&gt;
(picture) &lt;br /&gt;
&lt;br /&gt;
We also have to consider the number of loops so there are N/L loops so the loops per &amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt; is (N/L)&amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt;.&lt;br /&gt;
So from the magnetic field formula we have this so far: &lt;br /&gt;
&lt;br /&gt;
(picture)&lt;br /&gt;
&lt;br /&gt;
Step 3: Add Up the Contributions of All the Pieces.&lt;br /&gt;
Turn the equation we have so far into an integral and solve out the integral. &lt;br /&gt;
&lt;br /&gt;
(picture)&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
Solenoids have many applications and they are a very common aspect of our daily lives. They can be found in electric locking mechanisms, medical equipment, cars, air conditioning systems, as well as many other devices. &lt;br /&gt;
To learn more about the applications of Solenoids in detail, you can go to this internal link: [[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of a Loop]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14342</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14342"/>
		<updated>2015-12-05T17:12:23Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the &amp;lt;math&amp;gt;\Delta \vec{B}&amp;lt;/math&amp;gt;,&lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
(picture)&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable &amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt;, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
&lt;br /&gt;
(picture) &lt;br /&gt;
&lt;br /&gt;
We also have to consider the number of loops so there are N/L loops so the loops per &amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt; is (N/L)&amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt;.&lt;br /&gt;
So from the magnetic field formula we have this so far: &lt;br /&gt;
&lt;br /&gt;
(picture)&lt;br /&gt;
&lt;br /&gt;
Step 3: Add Up the Contributions of All the pieces &lt;br /&gt;
==Connectedness==&lt;br /&gt;
Solenoids have many applications and they are a very common aspect of our daily lives. They can be found in electric locking mechanisms, medical equipment, cars, air conditioning systems, as well as many other devices. &lt;br /&gt;
To learn more about the applications of Solenoids in detail, you can go to this internal link: [[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of a Loop]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14339</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14339"/>
		<updated>2015-12-05T17:10:58Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the &amp;lt;math&amp;gt;\Delta \vec{B}&amp;lt;/math&amp;gt;,&lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
(picture)&lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable &amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt;, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
&lt;br /&gt;
(picture) &lt;br /&gt;
&lt;br /&gt;
We also have to consider the number of loops so there are N/L loops so the loops per &amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt; is (N/L)&amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt;.&lt;br /&gt;
So from the magnetic field formula we have this so far: &lt;br /&gt;
&lt;br /&gt;
(picture)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
Solenoids have many applications and they are a very common aspect of our daily lives. They can be found in electric locking mechanisms, medical equipment, cars, air conditioning systems, as well as many other devices. &lt;br /&gt;
To learn more about the applications of Solenoids in detail, you can go to this internal link: [[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of a Loop]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14319</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14319"/>
		<updated>2015-12-05T17:04:34Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the &amp;lt;math&amp;gt;\Delta \vec{B}&amp;lt;/math&amp;gt;,&lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable &amp;lt;math&amp;gt;\Delta \vec{x}&amp;lt;/math&amp;gt;, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
We also have to consider the number of loops so there are N/L loops so the loops per &amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt; is (N/L)&amp;lt;math&amp;gt;\Delta {x}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of a Loop]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14317</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14317"/>
		<updated>2015-12-05T17:03:55Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the &amp;lt;math&amp;gt;\Delta \vec{B}&amp;lt;/math&amp;gt;,&lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable &amp;lt;math&amp;gt;\Delta \vec{x}&amp;lt;/math&amp;gt;, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
We also have to consider the number of loops so there are N/L loops so the loops per &amp;lt;math&amp;gt;\Delta \vec{x}&amp;lt;/math&amp;gt; is (N/L)&amp;lt;math&amp;gt;\Delta \vec{L}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of a Loop]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14315</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14315"/>
		<updated>2015-12-05T17:02:32Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the &amp;lt;math&amp;gt;/Delta B&amp;lt;/math&amp;gt; &lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable x, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
We also have to consider the number of loops so there are N/L loops so the loops per &amp;lt;math&amp;gt;{delta}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of a Loop]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14309</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14309"/>
		<updated>2015-12-05T16:59:56Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the |Delta|B &lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable x, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
We also have to consider the number of loops &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
&lt;br /&gt;
[[Right Hand Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Magnetic Field of a Loop]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14308</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14308"/>
		<updated>2015-12-05T16:59:11Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the |Delta|B &lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable x, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
We also have to consider the number of loops &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
[[Ampere&#039;s Law]]&lt;br /&gt;
[[Right Hand Rule]]&lt;br /&gt;
[[Magnetic Field of a Loop]]&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14306</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14306"/>
		<updated>2015-12-05T16:58:46Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Created by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
To determine the direction of the magnetic field: use your right hand and curl your fingers towards the direction of the current and the direction that your thumb is pointing to is the direction of the magnetic field. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the |Delta|B &lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable x, which is given by the location of a single piece. d-x is given by the distance from the loop to the observation location.  &lt;br /&gt;
We also have to consider the number of loops &lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
[[Solenoid Applications]]&lt;br /&gt;
Ampere&#039;s Law&lt;br /&gt;
Right Hand Rule&lt;br /&gt;
Magnetic Field of a Loop&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14272</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14272"/>
		<updated>2015-12-05T16:38:23Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
This formula is used inside a long solenoid, when the radius of the solenoid is much smaller than the length. &lt;br /&gt;
B is the magnetic field. &lt;br /&gt;
&amp;lt;math&amp;gt;{\mu _{0}}&amp;lt;/math&amp;gt; is a constant.&lt;br /&gt;
N is the number of loops in the solenoid.&lt;br /&gt;
L is the length of the solenoid. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the |Delta|B &lt;br /&gt;
Think about this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Equation for the Magnetic Field Because of One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
We find the integration variable &lt;br /&gt;
&lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
A simple example of this &lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14253</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=14253"/>
		<updated>2015-12-05T16:26:08Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
&lt;br /&gt;
Step 1: Cut up the distribution into pieces and Draw the |Delta|B &lt;br /&gt;
Consider this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
We want to find the magnetic field contributed by each of the loops at any location along the axis of the solenoid. &lt;br /&gt;
&lt;br /&gt;
Step 2: Write an Expression for the Magnetic Field Due to One Piece. &lt;br /&gt;
The origin is located at the center of the solenoid. &lt;br /&gt;
[[File:solenoid.jpg]]&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=12043</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=12043"/>
		<updated>2015-12-04T17:08:31Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To solve for the magnetic field of a solenoid, you can use a four step process. &lt;br /&gt;
Step: Cut up the distribution into pieces and Draw the |Delta|B &lt;br /&gt;
Consider this: a solenoid the length of L that&#039;s made up for N circular loops tightly wound, each with a radius of R and a conventional current in the loops is I. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=12022</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=12022"/>
		<updated>2015-12-04T16:41:13Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt;  B = {\mu _{0}} \frac{NI}{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=12017</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=12017"/>
		<updated>2015-12-04T16:37:39Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt; B = \frac{\mu _{0}\cdot \frac{NI }{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=12016</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=12016"/>
		<updated>2015-12-04T16:37:24Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
A Solenoid is a type of electromagnet, which consists of a coil tightly wound into a helix. Usually it produces a uniform magnetic field when an electric current is run through it. The purpose of a solenoid is to create a controlled magnetic field. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The purpose of this application is to explore another way to apply the Biot-Sarvart law. The magnetic field is uniform along the axis of the solenoid, when electric current is run through it. The solenoid has has to have coils much larger than the radius. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
This is the formula for the magnetic field inside a long solenoid: &lt;br /&gt;
&amp;lt;math&amp;gt; B = \frac{\mu _{0}}{4\pi }\cdot \frac{NI }{L}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=11723</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=11723"/>
		<updated>2015-12-04T06:22:20Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
Short Description of Topic&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
State, in your own words, the main idea for this topic&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]&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;
[[Category:Which Category did you place this in?]]&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=4897</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=4897"/>
		<updated>2015-11-30T22:12:37Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Contents [hide]&lt;br /&gt;
1 Magnetic Field of a Solenoid&lt;br /&gt;
1.1 A Mathematical Model&lt;br /&gt;
1.2 A Computational Model&lt;br /&gt;
2 Simple Example&lt;br /&gt;
2.1 Connectedness&lt;br /&gt;
2.2 History&lt;br /&gt;
2.3 See also&lt;br /&gt;
2.3.1 Further reading&lt;br /&gt;
2.3.2 External links&lt;br /&gt;
2.4 References&lt;br /&gt;
&lt;br /&gt;
Magnetic Field of Solenoid &lt;br /&gt;
&lt;br /&gt;
A Mathematical Model[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A Computational Model[edit]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Simple Example[edit]&lt;br /&gt;
Pathindependence.png&lt;br /&gt;
&lt;br /&gt;
In this example, the electric field is equal to E=(Ex,0,0). The initial location is A and the final location is C. In order to find the potential difference between A and C, we use dV=VC−VA.&lt;br /&gt;
&lt;br /&gt;
Since there are no y and z components of the electric field, the potential difference is dV=−(Ex∗(x1−0)+0∗(−y1−0)+0∗0)=−Ex∗x1&lt;br /&gt;
&lt;br /&gt;
BC.png&lt;br /&gt;
&lt;br /&gt;
Let&#039;s say there is a location B at (x1,0,0). Now in order to find the potential difference between A and C, we need to find the potential difference between A and B and then between B and C.&lt;br /&gt;
&lt;br /&gt;
The potential difference between A and B is dV=VB−VA=−(Ex∗(x1−0)+0∗0+0∗0)=−Ex∗x1.&lt;br /&gt;
&lt;br /&gt;
The potential difference between B and C is dV=VC−VB=−(Ex∗0+0∗(−y1−0)+0∗0)=0.&lt;br /&gt;
&lt;br /&gt;
Therefore, the potential difference A and C is VC−VA=(VC−VB)+(VB−VA)=Ex∗x1, which is the same answer that we got when we did not use location B.&lt;br /&gt;
&lt;br /&gt;
Connectedness[edit]&lt;br /&gt;
How is this topic connected to something that you are interested in?&lt;br /&gt;
How is it connected to your major?&lt;br /&gt;
Is there an interesting industrial application?&lt;br /&gt;
History[edit]&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
See also[edit]&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
Further reading[edit]&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
External links[edit]&lt;br /&gt;
Internet resources on this topic&lt;br /&gt;
&lt;br /&gt;
References[edit]&lt;br /&gt;
This section contains the the references you used while writing this page&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=4891</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=4891"/>
		<updated>2015-11-30T22:10:45Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;br /&gt;
&lt;br /&gt;
by Elisa Mercando&lt;br /&gt;
&lt;br /&gt;
Contents [hide] &lt;br /&gt;
1 Path Independence&lt;br /&gt;
1.1 A Mathematical Model&lt;br /&gt;
1.2 A Computational Model&lt;br /&gt;
2 Simple Example&lt;br /&gt;
2.1 Connectedness&lt;br /&gt;
2.2 History&lt;br /&gt;
2.3 See also&lt;br /&gt;
2.3.1 Further reading&lt;br /&gt;
2.3.2 External links&lt;br /&gt;
2.4 References&lt;br /&gt;
Path Independence[edit]&lt;br /&gt;
The potential difference between two locations does not depend on the path taken between the locations chosen.&lt;br /&gt;
&lt;br /&gt;
A Mathematical Model[edit]&lt;br /&gt;
In order to find the potential difference between two locations, we use this formula dV=−(Ex∗dx+Ey∗dy+Ez∗dz), where E is the electric field with components in the x, y, and z directions. Delta x, y, and z are the components of final location minus to the components of the initial location.&lt;br /&gt;
&lt;br /&gt;
A Computational Model[edit]&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here Teach hands-on with GlowScript&lt;br /&gt;
&lt;br /&gt;
Simple Example[edit]&lt;br /&gt;
Pathindependence.png&lt;br /&gt;
&lt;br /&gt;
In this example, the electric field is equal to E=(Ex,0,0). The initial location is A and the final location is C. In order to find the potential difference between A and C, we use dV=VC−VA.&lt;br /&gt;
&lt;br /&gt;
Since there are no y and z components of the electric field, the potential difference is dV=−(Ex∗(x1−0)+0∗(−y1−0)+0∗0)=−Ex∗x1&lt;br /&gt;
&lt;br /&gt;
BC.png&lt;br /&gt;
&lt;br /&gt;
Let&#039;s say there is a location B at (x1,0,0). Now in order to find the potential difference between A and C, we need to find the potential difference between A and B and then between B and C.&lt;br /&gt;
&lt;br /&gt;
The potential difference between A and B is dV=VB−VA=−(Ex∗(x1−0)+0∗0+0∗0)=−Ex∗x1.&lt;br /&gt;
&lt;br /&gt;
The potential difference between B and C is dV=VC−VB=−(Ex∗0+0∗(−y1−0)+0∗0)=0.&lt;br /&gt;
&lt;br /&gt;
Therefore, the potential difference A and C is VC−VA=(VC−VB)+(VB−VA)=Ex∗x1, which is the same answer that we got when we did not use location B.&lt;br /&gt;
&lt;br /&gt;
Connectedness[edit]&lt;br /&gt;
How is this topic connected to something that you are interested in?&lt;br /&gt;
How is it connected to your major?&lt;br /&gt;
Is there an interesting industrial application?&lt;br /&gt;
History[edit]&lt;br /&gt;
Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.&lt;br /&gt;
&lt;br /&gt;
See also[edit]&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
Further reading[edit]&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
External links[edit]&lt;br /&gt;
Internet resources on this topic&lt;br /&gt;
&lt;br /&gt;
References[edit]&lt;br /&gt;
This section contains the the references you used while writing this page&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=4888</id>
		<title>Magnetic Field of a Solenoid</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Magnetic_Field_of_a_Solenoid&amp;diff=4888"/>
		<updated>2015-11-30T22:08:38Z</updated>

		<summary type="html">&lt;p&gt;Ramin8: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Claimed by ramin8 !!&lt;/div&gt;</summary>
		<author><name>Ramin8</name></author>
	</entry>
</feed>