faradays law of induction ap physics c montwood high school r. casao

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Faraday’s Law of Induction AP Physics C Montwood High School R. Casao

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Page 1: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Faraday’s Law of Induction

AP Physics C

Montwood High School

R. Casao

Page 2: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• Two simple experiments demonstrate that a current can be produced by a changing magnetic field.

• First: consider a loop of wire connected to a galvanometer as shown.

Page 3: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• If a magnet is moved toward the loop, the galvanometer needle will deflect in one direction.

Page 4: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• If a magnet is moved away from the loop, the galvanometer needle will deflect in the opposite direction.

Page 5: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• If the magnet is held stationary relative to the loop, no galvanometer needle deflection is observed.

Page 6: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• If the magnet is held stationary and the coil is moved toward or away from the magnet, the galvanometer needle will also deflect.

• From these observations, you can conclude that a current is set up in the circuit as long as there is relative motion between the magnet and the coil.

• This current is set up in the circuit even though there are no batteries in the circuit.

• The current is said to be an induced current, which is produced by an induced EMF.

Page 7: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Faraday’s Experiment• A coil is

connected to a switch and a battery.

• This is called the primary coil and the circuit is called the primary circuit.

• The coil is wrapped around an iron ring to intensify the magnetic field produced by the current through the coil.

Page 8: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Faraday’s Experiment• A second coil, on

the right, is wrapped around the iron ring and is connected to a galvanometer.

• This is secondary coil and the circuit is the secondary circuit.

• There is no battery in the secondary circuit and the secondary circuit is not connected to the primary coil.

Page 9: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Faraday’s Experiment• The only purpose

of this circuit is to detect any current that might be produced by a change in the magnetic field.

• When the switch in the primary circuit is closed, the galvanometer in the secondary circuit deflects in one direction and then returns to zero.

Page 10: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Faraday’s Experiment• When the switch is

opened, the galvanometer deflects in the opposite direction and again returns to zero.

• The galvanometer reads zero when there is a steady current in the primary circuit.

Page 11: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• Faraday concluded that an electric current can be produced by a changing magnetic field.

• A current cannot be produced by a steady magnetic field.

• The current that is produced in the secondary circuit occurs for only an instant while the magnetic field through the secondary coil is changing.

• In effect, the secondary circuit behaves as though there were a source of EMF connected to it for a short instant.

• An induced EMF is produced in the secondary circuit by the changing magnetic field.

Page 12: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• In both experiments, an EMF is induced in a circuit when the magnetic flux through the circuit changes with time.

• Faraday’s Law of Induction: The EMF induced in a circuit is directly proportional to the time rate of change of magnetic flux through the circuit.

– where Φm is the magnetic flux threading the circuit.

– Magnetic flux Φm :

dtdΦ

EMF m

dABΦm

Page 13: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• The integral of the magnetic flux is taken over the area bounded by the circuit.

• The negative sign is a consequence of Lenz’s law and is discussed later (the induced EMF opposes the change in the magnetic flux in the circuit).

• If the circuit is a coil consisting of N loops all of the same area and if the flux threads all loops, the induced EMF is:

dtdΦ

NEMF m

Page 14: Faradays Law of Induction AP Physics C Montwood High School R. Casao

dt

θ cosABd-EMF

• Suppose the magnetic field is uniform over a loop of area A lying in a plane as shown in the figure below.

• The flux through the loop is equal to B·A·cos ; and the induced EMF is:

Page 15: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• An EMF can be induced in the circuit in several ways:

1. The magnitude of B can vary with time;

2. The area of the circuit can change with time;

3. The angle between B and the normal to the plane can change with time; and

4. Any combination of these can occur.

Page 16: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Application of Faraday’s Law• A coil is wrapped with 200 turns of wire on the

perimeter of a square frame of sides 18 cm. Each turn has the same area, equal to that of the frame, and the total resistance of the coil is 2 . A uniform magnetic field is turned on perpendicular to the plane of the coil. If the field changes linearly from 0 to 0.5 Wb/m2 in a time of 0.8 s, find the magnitude of the induced EMF in the coil while the field is changing.– Loop area = (0.18 m)2 = 0.0324 m2

– At t = 0 s, the magnetic flux through the loop is 0 since B = 0 T.

Page 17: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Application of Faraday’s Law– At t = 8 s, the magnetic flux through the loop is

Φm = B·A = 0.5 Wb/m2·0.0324 m2 = 0.0162 Wb.

– The magnitude of the induced EMF is:

V4.05EMF

s0s0.8Wb0Wb0.0162200

dtdΦN

EMF m

Page 18: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Exponentially Decaying B Field• A plane loop of wire of area A is placed in a

region where the magnetic field is perpendicular to the plane. The magnitude of B varies in time according to the expression B = Bo·e-a·t. That is, at t = 0 s, the field is Bo, and for t > 0, the field decreases exponentially in time. Find the induced EMF in the loop as a function of time.– At t = 0 s, B is perpendicular to the plane of the loop

and is a maximum.– The magnetic flux through the loop at time t > 0 is:

AeBABΦ atom

Page 19: Faradays Law of Induction AP Physics C Montwood High School R. Casao

aeABEMFdtdt

aeABEMF

dttad

eABEMF

dted

ABdtdΦ

EMF

tao

tao

tao

ta

om

Page 20: Faradays Law of Induction AP Physics C Montwood High School R. Casao

Applications of Faraday’s Law

• The ground fault interrupter (GFI) is a safety device that protects users of electrical appliances against electric shock by making use of Faraday’s law.

• Wire 1 leads from the wall outlet to the appliance to be protected.• Wire 2 leads from the appliance back to the wall outlet.

Page 21: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• An iron ring surrounds the two wires, and a sensing coil is wrapped around part of the ring.

• Because the currents in the wires are in opposite directions, the net magnetic flux through the sensing coil due to the currents is zero.

• If the return current in wire 2 changes, the net magnetic flux thru the sensing coil is no longer zero.• This can happen if the appliance becomes wet, enabling the current to leak to the ground.

Page 22: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• Because household current is alternating (its direction keeps reversing), the magnetic flux through the sensing coil changes with time, inducing an EMF if the coil.

• The induced EMF is used to trigger a circuit breaker, which stops the current before it is able to reach a harmful level.

Electric Guitar• The coil is called a pickup coil and is placed near

the vibrating guitar string, which is made of a metal that can be magnetized.

• A permanent magnet inside the coil temporarily magnetizes the portion of string nearest the coil.

Page 23: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• When the string vibrates at some frequency, its magnetized section produces a changing magnetic flux thru the coil.

Page 24: Faradays Law of Induction AP Physics C Montwood High School R. Casao

• The changing flux induces an EMF in the pickup coil that is fed to an amplifier.

• The output of the amplifier is sent to the speakers, which produce the sound we hear.

Page 25: Faradays Law of Induction AP Physics C Montwood High School R. Casao

A Note on the Magnitude of an Induced Current

• The induced current in the conducting loop has the same magnitude at all points in the loop.