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'''Claimed by Jenny Zang (Fall 2016)'''
"Edited by Alex Casado (Spring 2019)"


'''Edited by Halle Bryan (Fall 2016)'''


Formulated in 1834, Lenz's Law helps determine the direction of current and the field is creates. When an induced current is generated by a change in magnetic flux, as stated by Farady's Law, the induced current will flow creating its own magnetic field that opposes the magnetic field that created it. Lenz's Law and Faraday's Law of Induction are highly connected, with the negative sign in Faraday's Law showing Lenz's Law. The current direction is important in the upholding of the conservation of energy. Lenz's Law is connected to this conservation and therefore Newton's Third Law as well. 
==The Main Idea==


==The Main Idea==
Lenz's Law is applies the law of conservation of energy to Faraday's Law, which states that any change in the magnetic field will cause an induced current. Lenz's law accounts for the direction of the new current - with the change coming from either the strength of the magnetic field, the direction of the magnetic field, the position of a circuit, the shape of a circuit, or the orientation of a circuit. To keep the magnetic flux of a loop of wires constant, there is an induced magnetic field. Change in magnetic flux results in an equal and opposite change in the loop which is why we use negative <math>{\frac{dB}{dt}}</math>. Below is a basic visualization of Lenz's Law where there is an existing magnetic field.
 
[[File:lenzlaw1.png]]
(image obtained from https://brilliant.org/wiki/lenzs-law/)
 
This Law is applied to determine the direction of current and the field it creates. When an induced field is generated by a change in magnetic flux (Faraday's Law), the induced current will flow creating its own magnetic field that opposes the magnetic field that created it. Direction is important when dealing with the law of conservation of energy. It can be seen applied when looking at electromagnetism such as the direction of voltage induced in an inductor.
 
In summary, whenever there is a change in magnetic flux in a conducting loop, the charge is balanced by the induction of a magnetic field. The integral of B * n remains constant.


Lenz's Law makes sure that Faraday's Law follows the conservation of energy as stated by Newton's Third Law. According to Faraday's Law, any change a the magnetic field will cause an induced current (emf). Lenz's Law accounts for the direction of the induced current. The change can be caused by the strength of the magnetic field, the direction of the magnetic field, the position of a circuit, the shape of a circuit, or the orientation of a circuit. The induced magnetic field inside a loop of wires is created to keep the magnetic flux in the loop constant. This graphic displays a basic understanding of how Lenz's Law could function in one example:
==Theory==
[[File:Flow Chart.jpg]]


===A Mathematical Model===
===Mathematical Model===


Lenz's Law is mathematically modeled as part of Faraday's Law. The negative sign in the equation represents the opposing induced field.  
Lenz's Law is mathematically modeled as part of Faraday's Law. The negative sign in the equation represents the opposing induced field.  
<math>\epsilon = -{\frac{d\phi}{dt}} </math> where '''<math>\epsilon</math>''' is the emf of the system and '''<math>d\phi</math>''' is the change in the magnetic field.
<math>\epsilon = -{\frac{d\phi}{dt}} </math> where '''<math>\epsilon</math>''' is the emf of the system and '''<math>d\phi</math>''' is the change in the magnetic field. This means the induced electromotive force and rate of change in magnetic flux both have opposite signs. While there is a formula, it is important to note that this is mainly a qualitative law and does not incorporate magnitude, only direction.


===A Computational Model===
Example:
The currents seen within strong magnets can create currents rotating in the opposite direction in metals like cooper or aluminum. If you were to drop a strong magnet through a cooper or aluminum pipe, you would observe that the velocity is decently slower than if you were to drop the magnet outside of the pipe.


https://www.youtube.com/watch?v=xxZenoBs2Pg This links to a video by Khan Academy that explains how Lenz's Law works through an example.
=== Right Hand Rule ===
 
The Right Hand Rule is a heuristic used to determine the direction of angular momentum as a vector. The direction of angular momentum is determined by calculating the cross product of the vectors. To use the Right Hand Rule, place your thumb in the direction of <math> -dB </math> and curl your fingers. The direction of the non-coulombic electric field is the same direction as your fingers curl. An example of how the cross product is performed is below.


https://www.youtube.com/watch?v=Vs3afgStVy4 This links to a video by Grand Illusions that displays Lenz's Law using a magnetic falling down a tube.
[[File:Crossproductcasado.png]]


==Examples==
==Examples==
'''Example 1'''
'''Right Hand Rule'''


Use the right hand rule to find the non-coulombic electric field in the given situations.
In the examples above, the direction of the electric field is the pink arrows. This can be determined by first placing your thumb in the direction of the <math> -dB </math> and then curling your fingers. The direction your fingers curl is the direction of the electric field.
[[File:Non-Coulobmic_Fields.gif]]
 
===Example 1: Easy===
 
A solenoid has current <math> I_1 </math> flowing around it increasing from 0 to 40A. A plain loop of wire is placed around the solenoid, perpendicular to the axis of the solenoid. An emf is produced, therefore producing an <math> I_2 </math>. Are <math> I_1 </math> and <math> I_2 </math> flowing in the same direction or opposite?


'''Solution'''
'''Solution'''


To use the right hand rule: place your thumb in the direction of the <math> -dB </math>, then curl your fingers. The direction in which your fingers curl is the direction of the non-coulombic electric field. The non-coulombic field is represented by the pink arrows.
The original current <math> I_1 </math> produced a magnetic field. In order to maintain the conservation of energy and Newton's Third Law, the magnetic field produced by <math> I_2 </math> must oppose this field. This is in accordance with Lenz's Law. Therefore, <math> I_2 </math> must oppose <math> I_1 </math> in direction.
 
 
===Example 2: Medium===


===Simple===
An magnet is moving through a copper tube (velocity drawn). Find the direction of -dB/dt and the direction of the induced current. Remember to use the right hand rule.


A solenoid has current <math> I_1 </math> flowing around it increasing from 0 to 40A. A plain loop of wire is placed around the solenoid, perpendicular to the axis of the solenoid. An emf is produced, therefore producing an <math> I_2 </math>. Are <math> I_1 </math> and <math> I_2 </math> flowing in the same direction or opposite?
[[File:LenzLaw.jpg]]
Graphic created by Nicole Romer


'''Solution'''
'''Solution'''
The original current <math> I_1 </math> produced a magnetic field. In order to maintain the conservation of energy and Newton's Third Law, the magnetic field produced by <math> I_2 </math> must oppose this field. This is in accordance with Lenz's Law. Therefore, <math> I_2 </math> must oppose <math> I_1 </math> in direction.


===Middling===
A)-y, clockwise B)+y, counterclockwise C)+y, counterclockwise D)-y, clockwise
[[File:Problem2.png]]
 
 
The magnetic field in this graphic is decreasing at a rate of 5.0mT/s. What is the direction of the current in the circle of wire?
 
[[File:hm235.jpg]]
 


'''Solution'''
'''Solution'''
The current in the circle of wire will produce a magnetic field that needs to supplement the existing diminishing field. This is in accordance with Lenz's Law. Therefore, the magnetic field produced needs to be into the page. Using the right hand rule, to produce a field going into the page the current in the circle of the wire must be in the clockwise direction.


===Difficult===
===Example 3: Difficult===
The magnetic field is decreasing at a rate of 5.0mT/s. The radius of the loop of wire is 5.0m, and the resistance is 5 ohms. What is the magnitude and direction of the current?
 
[[File:hm235.jpg]]


'''Solution'''
'''Solution'''
To find the magnitude of the current we must first use the formula <math>\epsilon = -{\frac{d\phi}{dt}} </math> to find the <math>\epsilon</math> representing the emf of the system. We know, more specifically, that <math>\epsilon = -NAcos\theta{\frac{d\phi}{dt}} </math>. Therefore, <math>\epsilon = -1*5.0^2*\pi*1*-5*10^{-3} </math> which resolves to <math>\epsilon = .392699</math>. From there, to find the current we know that <math>I = {\frac{\epsilon}{R}}</math>. Plugging in the values we know we find, <math>I = {\frac{.392699}{5.0}} = .07854A</math>. That is the magnitude of the current. To find the direction we must use Lenz's Law. The current in the circle of wire will produce a magnetic field that needs to supplement the existing diminishing field. Therefore, the magnetic field produced needs to be into the page. Using the right hand rule, to produce a field going into the page the current in the circle of the wire must be in the clockwise direction.


==Connectedness==
==Connectedness==
An interesting application for Lenz's Law is to cause rotation to create energy. In an industry setting, Lenz's Law can be applied to electric generators or electric motors. When a current is induced in a generator, the direction of the induced current will flow in opposition of the magnetic field that created it, causing rotation of the generator. And so, the generator needs more mechanical energy.
 
An application of Lenz's Law is to cause rotation to create energy. In industry, Lenz's Law can be applied to electric generators or motors. When a current is induced in a generator, the direction of the induced current will flow in opposition of the magnetic field that created it. This causes rotation in the generator.
 
[[File:Electricmotor1.jpeg]]
 
Another application of Lenz's Law is in electromagnetic braking for vehicles. This process begins with electromagnets inducing eddy currents into the spinning rotor. Magnetic fields that oppose the initial change in magnetic flux are created from these eddy currents. This slows the rotor.
 
[[File:Electromagbraking.png]]
 
One last application of Lenz's Law is induction stove tops. These cooktops heat up as a result of changing magnetic fields and eddy currents operating according to Lenz's Law.
 
[[File:inductionstove.jpeg]]


==History==
==History==


Henrich Friefrich Emil Lenz (1804-1865), a Russian physicist of German origin was born in Dorpat, nowadays Tartu, Estonia. Henrich studied chemistry and physics at the University of Dorpat in 1820 after his secondary education. From 1823 to 1826, he traveled with the navigator, Otto von Kotzebue on his third expedition around the world. During this journey he studied climate conditions, and properties of seawater. After his travels, he worked at the University of St. Petersburg, Russia, where he later became the Dean of Mathematics and Physics from 1840 to 1863. In the year of 1831, he started studying electromagnetism, and soon after in 1835, what is known today as Lenz's Law was created. Lenz died on February 10, 1865, just two days before his 61st birthday, after suffering a stroke, while in Rome.
Henrich Friefrich Emil Lenz (1804-1865), a Russian physicist of German origin was born in Dorpat, nowadays Tartu, Estonia. Henrich studied chemistry and physics at the University of Dorpat in 1820 after his secondary education. From 1823 to 1826, he traveled with the navigator, Otto von Kotzebue on his third expedition around the world. During this journey he studied climate conditions, and properties of seawater. After his travels, he worked at the University of St. Petersburg, Russia, where he later became the Dean of Mathematics and Physics from 1840 to 1863. In the year of 1831, he started studying electromagnetism, and soon after in 1835, what is known today as Lenz's Law was created. Lenz was also know for carefully checking his work, testing any variable that might effect his results. Lenz died on February 10, 1865, just two days before his 61st birthday, after suffering a stroke, while in Rome.
 
== See also ==


Since Lenz's Law and Farady's Law go hand in hand, Faraday's Law would be great supplemental information to read about. Newton's Third Law would also be a topic to read on for further understanding why Lenz's Law exists.


===Further reading===
===Further reading===
Line 64: Line 97:
Conservation Laws
Conservation Laws
[http://hyperphysics.phy-astr.gsu.edu/hbase/conser.html]
[http://hyperphysics.phy-astr.gsu.edu/hbase/conser.html]
===More Videos For Study===
https://www.youtube.com/watch?v=xxZenoBs2Pg This links to a video by Khan Academy that explains how Lenz's Law works through an example.
https://www.youtube.com/watch?v=Vs3afgStVy4 This links to a video by Grand Illusions that displays Lenz's Law using a magnetic falling down a tube.


==References==
==References==

Latest revision as of 13:07, 14 April 2019

"Edited by Alex Casado (Spring 2019)"


The Main Idea

Lenz's Law is applies the law of conservation of energy to Faraday's Law, which states that any change in the magnetic field will cause an induced current. Lenz's law accounts for the direction of the new current - with the change coming from either the strength of the magnetic field, the direction of the magnetic field, the position of a circuit, the shape of a circuit, or the orientation of a circuit. To keep the magnetic flux of a loop of wires constant, there is an induced magnetic field. Change in magnetic flux results in an equal and opposite change in the loop which is why we use negative [math]\displaystyle{ {\frac{dB}{dt}} }[/math]. Below is a basic visualization of Lenz's Law where there is an existing magnetic field.

(image obtained from https://brilliant.org/wiki/lenzs-law/)

This Law is applied to determine the direction of current and the field it creates. When an induced field is generated by a change in magnetic flux (Faraday's Law), the induced current will flow creating its own magnetic field that opposes the magnetic field that created it. Direction is important when dealing with the law of conservation of energy. It can be seen applied when looking at electromagnetism such as the direction of voltage induced in an inductor.

In summary, whenever there is a change in magnetic flux in a conducting loop, the charge is balanced by the induction of a magnetic field. The integral of B * n remains constant.

Theory

Mathematical Model

Lenz's Law is mathematically modeled as part of Faraday's Law. The negative sign in the equation represents the opposing induced field. [math]\displaystyle{ \epsilon = -{\frac{d\phi}{dt}} }[/math] where [math]\displaystyle{ \epsilon }[/math] is the emf of the system and [math]\displaystyle{ d\phi }[/math] is the change in the magnetic field. This means the induced electromotive force and rate of change in magnetic flux both have opposite signs. While there is a formula, it is important to note that this is mainly a qualitative law and does not incorporate magnitude, only direction.

Example: The currents seen within strong magnets can create currents rotating in the opposite direction in metals like cooper or aluminum. If you were to drop a strong magnet through a cooper or aluminum pipe, you would observe that the velocity is decently slower than if you were to drop the magnet outside of the pipe.

Right Hand Rule

The Right Hand Rule is a heuristic used to determine the direction of angular momentum as a vector. The direction of angular momentum is determined by calculating the cross product of the vectors. To use the Right Hand Rule, place your thumb in the direction of [math]\displaystyle{ -dB }[/math] and curl your fingers. The direction of the non-coulombic electric field is the same direction as your fingers curl. An example of how the cross product is performed is below.

Examples

Right Hand Rule

In the examples above, the direction of the electric field is the pink arrows. This can be determined by first placing your thumb in the direction of the [math]\displaystyle{ -dB }[/math] and then curling your fingers. The direction your fingers curl is the direction of the electric field.

Example 1: Easy

A solenoid has current [math]\displaystyle{ I_1 }[/math] flowing around it increasing from 0 to 40A. A plain loop of wire is placed around the solenoid, perpendicular to the axis of the solenoid. An emf is produced, therefore producing an [math]\displaystyle{ I_2 }[/math]. Are [math]\displaystyle{ I_1 }[/math] and [math]\displaystyle{ I_2 }[/math] flowing in the same direction or opposite?

Solution

The original current [math]\displaystyle{ I_1 }[/math] produced a magnetic field. In order to maintain the conservation of energy and Newton's Third Law, the magnetic field produced by [math]\displaystyle{ I_2 }[/math] must oppose this field. This is in accordance with Lenz's Law. Therefore, [math]\displaystyle{ I_2 }[/math] must oppose [math]\displaystyle{ I_1 }[/math] in direction.


Example 2: Medium

An magnet is moving through a copper tube (velocity drawn). Find the direction of -dB/dt and the direction of the induced current. Remember to use the right hand rule.

Graphic created by Nicole Romer

Solution

A)-y, clockwise B)+y, counterclockwise C)+y, counterclockwise D)-y, clockwise


The magnetic field in this graphic is decreasing at a rate of 5.0mT/s. What is the direction of the current in the circle of wire?


Solution The current in the circle of wire will produce a magnetic field that needs to supplement the existing diminishing field. This is in accordance with Lenz's Law. Therefore, the magnetic field produced needs to be into the page. Using the right hand rule, to produce a field going into the page the current in the circle of the wire must be in the clockwise direction.

Example 3: Difficult

The magnetic field is decreasing at a rate of 5.0mT/s. The radius of the loop of wire is 5.0m, and the resistance is 5 ohms. What is the magnitude and direction of the current?

Solution

To find the magnitude of the current we must first use the formula [math]\displaystyle{ \epsilon = -{\frac{d\phi}{dt}} }[/math] to find the [math]\displaystyle{ \epsilon }[/math] representing the emf of the system. We know, more specifically, that [math]\displaystyle{ \epsilon = -NAcos\theta{\frac{d\phi}{dt}} }[/math]. Therefore, [math]\displaystyle{ \epsilon = -1*5.0^2*\pi*1*-5*10^{-3} }[/math] which resolves to [math]\displaystyle{ \epsilon = .392699 }[/math]. From there, to find the current we know that [math]\displaystyle{ I = {\frac{\epsilon}{R}} }[/math]. Plugging in the values we know we find, [math]\displaystyle{ I = {\frac{.392699}{5.0}} = .07854A }[/math]. That is the magnitude of the current. To find the direction we must use Lenz's Law. The current in the circle of wire will produce a magnetic field that needs to supplement the existing diminishing field. Therefore, the magnetic field produced needs to be into the page. Using the right hand rule, to produce a field going into the page the current in the circle of the wire must be in the clockwise direction.

Connectedness

An application of Lenz's Law is to cause rotation to create energy. In industry, Lenz's Law can be applied to electric generators or motors. When a current is induced in a generator, the direction of the induced current will flow in opposition of the magnetic field that created it. This causes rotation in the generator.

Another application of Lenz's Law is in electromagnetic braking for vehicles. This process begins with electromagnets inducing eddy currents into the spinning rotor. Magnetic fields that oppose the initial change in magnetic flux are created from these eddy currents. This slows the rotor.

One last application of Lenz's Law is induction stove tops. These cooktops heat up as a result of changing magnetic fields and eddy currents operating according to Lenz's Law.

History

Henrich Friefrich Emil Lenz (1804-1865), a Russian physicist of German origin was born in Dorpat, nowadays Tartu, Estonia. Henrich studied chemistry and physics at the University of Dorpat in 1820 after his secondary education. From 1823 to 1826, he traveled with the navigator, Otto von Kotzebue on his third expedition around the world. During this journey he studied climate conditions, and properties of seawater. After his travels, he worked at the University of St. Petersburg, Russia, where he later became the Dean of Mathematics and Physics from 1840 to 1863. In the year of 1831, he started studying electromagnetism, and soon after in 1835, what is known today as Lenz's Law was created. Lenz was also know for carefully checking his work, testing any variable that might effect his results. Lenz died on February 10, 1865, just two days before his 61st birthday, after suffering a stroke, while in Rome.


Further reading

Faraday's Law [1] Conservation Laws [2]

More Videos For Study

https://www.youtube.com/watch?v=xxZenoBs2Pg This links to a video by Khan Academy that explains how Lenz's Law works through an example.

https://www.youtube.com/watch?v=Vs3afgStVy4 This links to a video by Grand Illusions that displays Lenz's Law using a magnetic falling down a tube.

References

https://nationalmaglab.org/education/magnet-academy/history-of-electricity-magnetism/pioneers/heinrich-friedrich-emil-lenz http://hyperphysics.phy-astr.gsu.edu/hbase/conser.html http://regentsprep.org/regents/physics/phys08/clenslaw/ http://hyperphysics.phy-astr.gsu.edu/hbase/electric/farlaw.html http://farside.ph.utexas.edu/teaching/302l/lectures/node85.html http://www.electrical4u.com/lenz-law-of-electromagnetic-induction/