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This lesson covers Higher Tier content. Questions based on electromagnetic induction may appear only on Higher Tier papers in the Edexcel GCSE Combined Science specification (1SC0).
This lesson explains how a changing magnetic field can induce a voltage (and current) in a conductor, the factors that affect the size of the induced voltage and a qualitative understanding of Lenz's law.
Electromagnetic induction is the process of generating a voltage (and, if the circuit is complete, a current) in a conductor by changing the magnetic field around it.
There are two ways to induce a voltage:
| Method | Example |
|---|---|
| Move a conductor through a magnetic field | Pushing a wire between the poles of a magnet |
| Change the magnetic field around a stationary conductor | Moving a magnet into or out of a coil of wire |
In both cases, the conductor must cut through magnetic field lines (or the number of field lines passing through the coil must change).
A voltage is induced only while the magnetic field through the coil is changing. No change → no induced voltage.
Exam Tip: Students often lose marks by saying "moving a magnet induces a current." Be precise: the magnet must move relative to the conductor, and there must be a change in the magnetic field through the conductor.
| Factor | Effect of Increasing It |
|---|---|
| Speed of movement (magnet or wire) | Larger induced voltage |
| Strength of the magnet | Larger induced voltage |
| Number of turns on the coil | Larger induced voltage |
Doubling the speed, field strength or number of turns each produces a proportionally larger voltage.
Lenz's law states:
The direction of the induced current is always such that it opposes the change that produced it.
Lenz's law is a consequence of the conservation of energy — if the induced current aided the change, energy would be created from nothing.
graph LR
subgraph "Lenz’s Law — Magnet Pushed into Coil"
direction LR
Mag["N pole approaching →"] -->|"Induced N pole repels"| CoilEnd["Coil end becomes N"]
end
Exam Tip: Lenz's law is about opposition. The key word in any answer is "opposes." The induced effect always works against the change causing it.
When a magnet is repeatedly pushed in and out of a coil, the induced voltage alternates — it switches direction with each change of motion. This produces an alternating current (AC) if the circuit is complete.
| Motion | Voltage Direction |
|---|---|
| Magnet pushed in | One direction (e.g. positive) |
| Magnet stationary inside | Zero |
| Magnet pulled out | Opposite direction (e.g. negative) |
A student moves a bar magnet into a coil connected to a galvanometer. The galvanometer shows a deflection to the right. State and explain what happens if the student:
(a) Moves the magnet into the coil faster.
The galvanometer deflects further to the right — the induced voltage is larger because the rate of change of the magnetic field is greater.
(b) Holds the magnet stationary inside the coil.
The galvanometer reads zero — there is no change in the magnetic field, so no voltage is induced.
(c) Pulls the magnet out of the coil at the original speed.
The galvanometer deflects to the left — the direction of the change in magnetic field is reversed, so the induced voltage (and current) is in the opposite direction.
| Misconception | Correction |
|---|---|
| A stationary magnet inside a coil induces a voltage | No — the field must be changing for induction to occur |
| A stronger magnet always induces a larger current | Only if the magnet is moving relative to the conductor |
| Lenz's law means the induced current stops the magnet | The induced current opposes the motion but does not completely stop it (you still have to do work against the opposition) |
The modern way to describe induction uses magnetic flux (Φ), roughly "the amount of magnetic field passing through a loop." When the flux changes (by the field strength changing, by the loop changing area, or by the loop changing orientation), a voltage is induced. The induced EMF is proportional to the rate of change of flux:
ε=−NΔtΔΦ
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