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1 Physics 202 Chapter 31 Oct 23, 2007 Faraday’s Law Faraday’s Law The final step to ignite the industrial use of electromagnetism on a large scale. Light, toasters, cars, TVs, telephones, iPods, industrial production, …

Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Page 1: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Physics 202Chapter 31Oct 23, 2007

Faraday’s Law

Faraday’s Law

The final step toignite the industrialuse ofelectromagnetism ona large scale.

Light, toasters, cars,TVs, telephones,iPods, industrialproduction, …

Page 2: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Faraday’s Law “the emf induced in a circuit is directly proportional to

the time rate of change of the magnetic flux throughthe circuit”

ε= induced emf,

= induced potential difference

The induced emf is then: ε = - d/dt (BA cos θ)

In practice often: ΦB = BA cos θ

Faraday’s Law – Example Assume a loop

enclosing an area Alies in a uniformmagnetic field B

The magnetic fluxthrough the loop is ΦB = BA cos θ

The induced emf is ε = - d/dt (BA cos θ)

Page 3: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Ways of Inducing an emf The magnitude of B can change with time The area enclosed by the loop can change

with time The angle θ between B and the normal to

the loop can change with time Any combination of the above can occur

Lenz’s Law Faraday’s law indicates that the induced

emf and the change in flux have oppositealgebraic signs

Lenz’s law: the induced current in a loopis in the direction that creates amagnetic field that opposes the change inmagnetic flux through the area enclosedby the loop

Page 4: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Induced emf by changing B-field- a closer look

An increasing B-field generates acurrent.

That means electrons in the wire“see” a (circular) electric field.The E-field is not caused by astatic electric chargedistribution.

That means (in presence of achanging magnetic field):

Faraday’s law can be written ina general form:

!

E " ds# = $d%

B

dt

!

E " ds# $ 0

Examples on the whiteboard

Changing B-field Motional emf

Demonstration: Thesoda can crusher

Page 5: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Quick Quiz 31.2

The figure shows thetime dependence of auniform fiel B(t) thatpasses through a fixedloop and is orientedperpendicular to theplane of the loop.

Rank the magnitudes ofthe emf generated inthe loop at thefive instants indicated,fromlargest to smallest.

ε(t)

Quick Quiz 31.8

The figure below shows a circular loop of wire beingdropped toward a wire carrying a current to the left. Thedirection of the induced current in the loop of wire is

(a) clockwise

(b) counterclockwise

(c) zero

(d) impossible to determine

Page 6: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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QUICK QUIZ 31.3A square loop of wire is being pulled at a constant velocitythrough a region of uniform magnetic field pointing into thescreen.In the loop of wirea) there will be a current induced,b) charge separation will occur,c) a and b, ord) neither a nor b.

No Flux change!No induced field!No current!No force!

Animation here

Page 7: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Generators

Electric generatorstake in energy bywork and transfer itout by electricaltransmission

The AC generatorconsists of a loop ofwire rotated by someexternal means in amagnetic field

Applications of Faraday’s Law –Pickup Coil in electric guitar

A permanent magnet isplaced near the string ofthe guitar and causes aportion of the string tobecome magnetized

When the string vibratesat some frequency, themagnetized segmentproduces a changing fluxthrough the coil.

The induced emf is fed toan amplifier.

Page 8: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Rotating Loop Assume a loop with N

turns, The flux through the loop

at any time t is ΦB = BAcos θ = BA cos ωt

Resulting emf:

DC Generators

The DC (directcurrent) generatorhas essentially thesame components asthe AC generator

The main differenceis that the contactsto the rotating loopare made using asplit ring called acommutator

Page 9: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Motors

A motor is a generator operating inreverse

Eddy Currents

Circulating currents callededdy currents are induced inbulk pieces of metal movingthrough a magnetic field

The eddy currents are inopposite directions as theplate enters or leaves thefield

Eddy currents are oftenundesirable because theyrepresent a transformation ofmechanical energy intointernal energy

Page 10: Physics 202 Chapter 31 Oct 23, 2007karle/courses/phys202/202lecture15.pdf · Faraday’s law can be written in a general form:! #E"ds=$ d% B dt! #E"ds$0 Examples on the whiteboard

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Maxwell’s Equations,Introduction

Maxwell’s equations are regarded as thebasis of all electrical and magneticphenomena

Maxwell’s equations represent the laws ofelectricity and magnetism that havealready been discussed, but they haveadditional important consequences

Maxwell’s Equations

!

E " dAS

# =q

$0

B " dAS

# = 0

E " ds# = %d&B

dt

B " ds# = µ0I + $

0µ0

d&E

dt

Gauss’s law (electric)

Gauss’s law inMagnetism

Faraday’s Law

Ampere-Maxwell Law