Law of Electromagnetic Induction
Faraday’s Law of Induction
Faraday's Law of Induction states that the magnitude of the induced e.m.f. in a
circuit is directly proportional to the rate of change of magnetic field lines
cutting it.
The “rate” here is associated with the speed of the movement of magnet / coil.
When the speed changes, the magnitude of induced emf will change
accordingly.
Note that when the question does not mention about speed, we do not need to
explain the question with the “rate”. An explanation with “a change in magnetic
field lines cutting the coil” is sufficient.
The below illustration shows the meaning of a CHANGE in magnetic field lines
cutting the coil.
From position 1 to position 2, the number of magnetic field lines cutting the coil
changes from 1 to 5, hence, there is an increase (change) in the magnetic field
lines cutting the coil when the magnet moves from position 1 to position 2.
Thus, an emf is induced during this movement.
Note that when we know the change (either increase or decrease), we have to
state so.
The magnitude of induced emf can be increased by
• Increasing the number of turns in the solenoid per unit length
• Increasing the strength of magnet
• Move the magnet into or out the solenoid faster (look at question to see
whether magnet or solenoid is moving. Also, whether it moves in or out.
Then, change this factor accordingly.)
• Insert soft iron core into the solenoid
Lenz’s Law
Lenz's law states that the direction of the induced e.m.f. (and hence induced
current in a closed circuit) is always such that its magnetic effect opposes the
change producing it.
By Lenz’s Law, when magnet is inserted into the solenoid, a North pole will be
induced on the right side of coil to oppose the incoming North pole. By Right
Hand Grip Rule, the induced current will flow anticlockwise so that pointer
deflects to right.
By Lenz’s Law, when magnet is withdrawn from the solenoid, a South pole will
be induced on the right side of coil to oppose the outgoing North pole. By Right
Hand Grip Rule, the induced current will flow clockwise so that pointer deflects
to left.
Note that although the direction of induced emf opposes the change producing
it, it still occurs. This means the magnet will still go into the solenoid or leave
the solenoid, but it takes a little bit longer due to opposing force.
The following analogy might help to understand the Lenz’s Law better.
• For example, your class is very united and close. Suddenly one student
wants to study overseas, you will try to oppose this and wish him to stay.
Nevertheless, he will still go overseas.
• Likewise, when another student suddenly transfers into your class, you
try to against this initially, and yet the student still joins your class.
Note:
• Faraday’s Law gives the magnitude of induced emf while Lenz’s
Law gives the direction of the induced emf.
• Lenz’s Law is an example of principle of Conservation of
Energy. Mechanical work is done to against the opposing force
experienced by the moving magnet, and this work is converted into
electrical energy as indicated by induced current flowing in the circuit.
Example:
(a) Explain why an emf is induced when the coil
moves into the magnet.
(b) Explain the direction of induced current in the
coil.
(c) Explain the effect on the magnitude of the
induced current when moving the coil more slowly.
Answer:
(a) As the coil moves into the magnet, there is an increase in the magnetic
field lines cutting the coil. By Faraday’s Law, this induces an e.m.f. across the
coil (which drives an induced current (include this only if question asks for
induced current)).
(b) By Lenz’s Law, the direction of induced current always opposes the change
producing it. Thus, North pole is induced on the left side of coil when it moves
towards North pole of magnet. By Right Hand Grip Rule, the induced current
flows clockwise in the coil
(c) If the coil is moved more slowly, there is a decrease in the rate of
change of magnetic field lines cutting the coil. Thus, the magnitude of the
induced current decreases, which is shown by a smaller deflection of the
galvanometer.
