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Electro- magnetic Induction Lecture 3 AP Physics

Electro- magnetic Induction Lecture 3 AP Physics

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Page 1: Electro- magnetic Induction Lecture 3 AP Physics

Electro-magnetic Induction

Lecture 3 AP Physics

Page 2: Electro- magnetic Induction Lecture 3 AP Physics

Class Demo

Producing a voltage with a magnetic field and a wire coil.

Page 3: Electro- magnetic Induction Lecture 3 AP Physics

Result

A voltage is produced by a changing magnetic field in a coil of wire

We will call this voltage an emfemf (electro-motive-force) to remind us that it is induced by magnetism.

Page 4: Electro- magnetic Induction Lecture 3 AP Physics

Faraday

Michael Faraday (1791-1867)

The experimentalist of 1800’s

Invented motor, generator, transformer, electrolysis and the theory of electromagnetic induction

Page 5: Electro- magnetic Induction Lecture 3 AP Physics

Magnetic Flux

The voltage created depends on the magnetic field and the area

B A ����������������������������

Page 6: Electro- magnetic Induction Lecture 3 AP Physics

Magnetic Flux

cos

B A

BA

Page 7: Electro- magnetic Induction Lecture 3 AP Physics

Faraday’s Law of Induction

The instantaneous induced emf equals the rate of change of the magnetic flux through the circuit

Nt

Page 8: Electro- magnetic Induction Lecture 3 AP Physics

Lenz’s Law

The polarity of the induced emf is such that it produces a current whose magnetic field opposesopposes the change in the magnetic flux.

Page 9: Electro- magnetic Induction Lecture 3 AP Physics

Lenz’s Law

Page 10: Electro- magnetic Induction Lecture 3 AP Physics

Example

200 turn square coil, 18 cm on a side had a resistance of 2 . Find the emf and current in the loop if the perpendicular magnetic field changes from 0 to 0.5 T in 0.8 sec.

4.05 V

2.03 A

Nt

IR

Page 11: Electro- magnetic Induction Lecture 3 AP Physics

Motional emf

An emf will be produced any time there is relative motion between the circuit and the field.

Page 12: Electro- magnetic Induction Lecture 3 AP Physics
Page 13: Electro- magnetic Induction Lecture 3 AP Physics

Motional emf

B v

Page 14: Electro- magnetic Induction Lecture 3 AP Physics

Generators

Page 15: Electro- magnetic Induction Lecture 3 AP Physics

Generators

The emf varies sinusoidally

Depends on the number of loops, the magnetic field, the size of the loop and the angular velocity

Page 16: Electro- magnetic Induction Lecture 3 AP Physics

Generators

sinNBA t

max NBA

Page 17: Electro- magnetic Induction Lecture 3 AP Physics

The Motor

A motor converts electrical energy to mechanical energy

A generator converts mechanical energy to electrical energy

Page 18: Electro- magnetic Induction Lecture 3 AP Physics

Eddy Currents

Demo: falling magnet

Page 19: Electro- magnetic Induction Lecture 3 AP Physics

Self Inductance

Page 20: Electro- magnetic Induction Lecture 3 AP Physics

Self-inductance

A coil will oppose any change in the magnetic flux.

If there is a change, there will be an induced emf that will oppose the change. (Lenz’s Law)

This opposition to change is called the self-self-inductanceinductance of the circuit

Self-inductance is like inertia: it opposes any change in the current. Applet: http://www.walter-fendt.de/ph14e/osccirc.htm

Page 21: Electro- magnetic Induction Lecture 3 AP Physics

Self-inductance

Induced voltage is related to the rate

the current is changing: I

Lt

The inductance is the constant of

proportionality: N

LI

Page 22: Electro- magnetic Induction Lecture 3 AP Physics

Self-inductance

Unit of self-inductance is the Henry

V s1 H 1

A

Page 23: Electro- magnetic Induction Lecture 3 AP Physics

Self-inductance

For a solenoid, N turns and length l, the self inductance is

2oN A

L

Page 24: Electro- magnetic Induction Lecture 3 AP Physics

Energy

Energy is stored in an inductor

21

2PE L I

Page 25: Electro- magnetic Induction Lecture 3 AP Physics

Links

Additional Links:http://www.physics.sjsu.edu/becker/physics51/induction.htm

http://hyperphysics.phy-astr.gsu.edu/HBASE/magnetic/magcon.html#c1