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Faraday’s Law of Induction

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Faraday s 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. – PowerPoint PPT presentation

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Title: Faraday’s Law of Induction


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

2
  • 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.

3
  • If a magnet is moved toward the loop, the
    galvanometer needle will deflect in one
    direction.

4
  • If a magnet is moved away from the loop, the
    galvanometer needle will deflect in the opposite
    direction.

5
  • If the magnet is held stationary relative to the
    loop, no galvanometer needle deflection is
    observed.

6
  • 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.

7
Faradays 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.

8
Faradays 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.

9
Faradays 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.

10
Faradays 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.

11
  • 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.

12
  • In both experiments, an EMF is induced in a
    circuit when the magnetic flux through the
    circuit changes with time.
  • Faradays 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 Fm is the magnetic flux threading the
    circuit.
  • Magnetic flux Fm

13
  • The integral of the magnetic flux is taken over
    the area bounded by the circuit.
  • The negative sign is a consequence of Lenzs 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

14
  • 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 BAcos ?
    and the induced EMF is

15
  • An EMF can be induced in the circuit in several
    ways
  • The magnitude of B can vary with time
  • The area of the circuit can change with time
  • The angle ? between B and the normal to the plane
    can change with time and
  • Any combination of these can occur.

16
Application of Faradays 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.

17
Application of Faradays Law
  • At t 8 s, the magnetic flux through the loop is
    Fm BA 0.5 Wb/m20.0324 m2 0.0162
    Wb.
  • The magnitude of the induced EMF is

18
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 Boe-at. That
    is, at t 0 s, the field is Bo, and for t gt 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 gt 0
    is

19
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20
Applications of Faradays Law
  • The ground fault interrupter (GFI) is a safety
    device that protects users of electrical
    appliances against electric shock by making use
    of Faradays 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.

21
  • 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.

22
  • 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.

23
  • When the string vibrates at some frequency, its
    magnetized section produces a changing magnetic
    flux thru the coil.

24
  • 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.

25
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.
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