Lenz's law: direction and energy

Key idea: An induced current produces a magnetic effect opposing the change that caused it. The mechanical work needed against that effect supplies electrical energy, consistent with energy conservation.

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  • GCE A-Level H2 Physics 2027
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Faraday’s law gives the size of an induced e.m.f.; Lenz’s law gives its direction. The rule is short, but it is easy to misread: the induced current opposes the change in flux, not the flux itself. Behind it is the conservation of energy.

Lenz’s law

Lenz’s law: the direction of the induced e.m.f. is such that it tends to oppose the change producing it. In a closed coil, the induced current sets up its own magnetic field, and that field opposes the change in flux linkage.

To find the direction of the induced current in a coil:

  1. Say which side you are viewing the coil from, and find the direction of the external flux through it.
  2. Decide whether that flux is increasing or decreasing.
  3. Choose the direction of the induced field that opposes the change: opposite to the external field if the flux is increasing, the same way if it is decreasing.
  4. Use the right-hand grip rule: an anticlockwise current gives a field towards you, a clockwise current a field away from you.
Lenz's law with a defined viewing directionLeft: a north pole moves right towards a coil, increasing rightward external flux. Right: viewed from the magnet towards the coil, anticlockwise induced current gives a field out of the page and makes the near face north. The coil belongs to a closed resistive circuit; its connections are omitted.North pole approachesSNmotioncoilrightward external flux increasesViewed from the magnetnear face: Ninduced B out of page (•)external flux into page increases
Lenz's law with a defined viewing directionLeft: a north pole moves right towards a coil, increasing rightward external flux. Right: viewed from the magnet towards the coil, anticlockwise induced current gives a field out of the page and makes the near face north. The coil belongs to a closed resistive circuit; its connections are omitted.North pole approachesSNmotioncoilrightward external flux increasesViewed from the magnetnear face: Ninduced B out of page (•)external flux into page increases
Viewed from the approaching north pole, anticlockwise current makes the coil’s near face north, opposing increasing inward flux. The closed-circuit diagram is not to scale.

Viewed from a north pole approaching a coil, the external flux points into the coil, away from you, and is increasing. The induced field points towards you, so the current is anticlockwise and the near face of the coil is a north pole, repelling the magnet. When the north pole is pulled away, the inward flux decreases; the induced field is inward, the current clockwise and the near face a south pole, attracting the magnet back.

Lenz investigation, viewed from the magnet’s side. North pole faces the coil. The magnet is held still; induced current is zero. Current equals e.m.f. divided by resistance; self-inductance is neglected.

Magnet motion
Current, viewed from magnet
zero
Motion
held still
Induced e.m.f.
0 mV
Current in the meter
0 mA
Magnet speed
0.00 m/s
Induced e.m.f. against time

Try this

0 of 1 done
  1. Predict each direction, then play Approach, Hold still and Withdraw with the same pole facing the coil. (not done yet)

The magnet stays on the near side of a closed coil, and directions are viewed from the magnet’s side. The model uses ε = -d(NΦ)/dt and I = ε/R, and ignores the coil’s self-inductance. On Hold the magnet stops at once, so the current is zero even though flux still links the coil. The meter needle may take a moment to settle; that is not current lingering.

Worked example 1

A weakening field

Problem

A closed loop lies in the plane of the page. A uniform magnetic field through it points out of the page and is decreasing. Find the direction of the induced current, as seen on the page.

Show full solution
  1. The change

    Method

    State the direction of the flux and how it is changing.

    Reason

    Lenz’s law responds to the change, not to the field itself.

    Working

    Answer

    The flux out of the page is decreasing.

  2. Induced field

    Method

    Choose the field that opposes the decrease.

    Reason

    To resist a fall in outward flux, the loop adds outward flux of its own.

    Working

    Answer

    The induced field is out of the page, the same direction as the external field.

  3. Current

    Working

    Answer

    By the right-hand grip rule, a field out of the page comes from an anticlockwise current.

Guided practice 2

Increasing, then steady

About 2 min

Problem

A magnetic field out of the page is increasing through a closed coil lying in the page. Which way is the induced current, as seen on the page? What is the current once the field stops changing? Treat the circuit as resistive with negligible self-inductance.

Find the current

While the field increases
Once the field is steady

Hints

Hint 1

oppose, then grip

The outward flux is growing. Choose the opposing induced field, then use the grip rule.

Show full solution
  1. Current

    Working

    Answer

    The induced field is into the page, so the current is clockwise. Once the field is steady, the flux is not changing and there is no current in the stated resistive model.

Spot the mistake 3

“The current is clockwise”

About 2 min

Learner claim

A coil has a north pole on the face nearest a magnet. A student says “the current is clockwise” without saying where the coil is viewed from. Which way is the current seen from the magnet’s side, and from the other side?

Try this before viewing the solution

Seen from the magnet's side
Seen from the other side

Show solution step by step
  1. From the north face

    Method

    Use the grip rule with the field pointing towards you.

    Reason

    Field lines leave a north face, so from that side the coil’s field points at the viewer.

    Working

    Answer

    Anticlockwise

  2. From the other side

    Working

    Answer

    Clockwise. The current itself has not changed.

Lenz’s law and energy

Lenz’s law follows from the conservation of energy. When a magnet is pushed towards a closed coil, the induced current makes the near face of the coil repel it. You have to do work to keep the magnet moving, and that work becomes the electrical energy in the coil, which ends up heating it.

If the induced current had the opposite direction, the coil would attract the magnet and speed it up. The magnet would then gain kinetic energy and the coil would gain electrical energy, both from nothing. That cannot happen, so the induced current must oppose the change.

If the coil is not a complete circuit, an e.m.f. is still induced, but there is no current and so no opposing force.

Check your understanding 1

A magnet is moving towards a coil. The wire is cut so the coil becomes an open circuit while the magnet keeps moving. What happens to the induced e.m.f. and to the magnetic force from the induced current? Ignore brief switching effects and capacitance.

Induced e.m.f. while the magnet moves
Magnetic force from the induced current

Show answer

The changing flux still induces an e.m.f. across the open coil. With no complete path, there is no current, so the opposing force from that current disappears. Lenz’s law gives the direction in which the e.m.f. would drive a current if the circuit were closed.

Try it yourself 4

An approaching south pole

Minimal support

Problem

The south pole of a magnet is pushed towards a closed coil along its axis. Viewing the coil from the magnet’s side, find the pole on the near face of the coil and the direction of the induced current.

Find the pole and the current

Near face of the coil
Current, seen from the magnet

Hints

Hint 1

field lines

Field lines point towards a south pole, so the external flux through the coil points towards you and is increasing.

Show solution step by step
  1. Flux change

    Reason

    Field lines run into the approaching south pole, and they get stronger as it gets closer.

    Working

    Answer

    The flux towards the viewer is increasing.

  2. Pole and current

    Working

    Answer

    The induced field points away from the viewer, so the current is clockwise. Field lines enter the near face, so it is a south pole, which repels the approaching south pole.

Exam-style question 1

A withdrawing north pole

5 marks

Examination question

The north pole of a magnet is pulled away from a closed coil along its axis.

(a) State Lenz’s law. [1 mark]

(b) Viewing the coil from the magnet’s side, state the direction of the induced current and whether the coil attracts or repels the magnet. [2 marks]

(c) Explain, in terms of energy, why the coil must act on the magnet in this way. [2 marks]

Write your answer before viewing the mark scheme

Show solution step by step
  1. (a) Lenz's law

    1 mark

    Reason

    Use the standard wording.

    Working

    Answer

    The direction of the induced e.m.f. is such that it opposes the change producing it.

  2. (b) Current and force

    2 marks

    Method

    Find the flux change, oppose it, then use the grip rule.

    Reason

    The flux into the coil, away from the viewer, is decreasing, so the induced field also points away from the viewer.

    Working

    Answer

    The current is clockwise. The near face is a south pole, which attracts the magnet, opposing its withdrawal.

  3. (c) Energy

    2 marks

    Working

    Answer

    Work must be done against the attraction to pull the magnet away, and this work becomes the electrical energy in the coil. If the coil repelled the magnet instead, electrical energy and kinetic energy would both be gained from nothing, which breaks the conservation of energy.

Common mistakes

  • Saying the induced field always opposes the external field; it opposes the change in flux.
  • Giving “clockwise” or “anticlockwise” without saying where the coil is viewed from.
  • Expecting a current to continue after the flux has stopped changing.
  • Expecting an opposing force from a coil that is not a complete circuit.

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