Skip to content
Section III · Topic guide

Magnetic fields & induction

Section III — Sciences · a free, hand-written guide with worked reasoning and adaptive practice that finds your weak spots.

Used by applicants sitting in March & September

Your projected climb

DiagnosticTarget

Illustrative — once you start, your real projected score updates after every session.

Built forMarch & September sittings·GEMSAS & non-GEMSAS pathways·Domestic & international applicants·Australia · Ireland · UK

The short answer

Decide whether a changing magnetic set-up induces an EMF, which way it drives current, and what happens to the size of it when the conditions change.

Written and checked by GAMSAT tutors — not AI-generated.

Free interactive lesson

Try the reasoning style

Section I · Humanities & Social SciencesIllustrative example

We treat forgetting as a failure — a lapse to be patched with reminders and records. Yet a mind that kept everything could not think; it would drown in the undifferentiated noise of every moment it had ever lived. To forget is not so much to lose information as to decide, mostly without our noticing, what was never worth keeping.

The author's argument relies most directly on which unstated assumption?

Pick an option to see how the tutor reasons to the answer — not just whether you were right.

How to reason to the answer

Not quite — the answer is B.

Work backwards from the conclusion: a mind that ‘kept everything’ supposedly ‘could not think.’ That only follows if thinking means leaving most of experience out — so B is the premise the argument quietly rests on. A raises reliability, which the passage never weighs; C contradicts ‘mostly without our noticing’; D smuggles in a claim about intellect the passage never makes. The question rewards finding the hidden premise, not recalling a fact.

Section III hands you an apparatus you have never seen and asks: does anything happen, which way, and how big? Forces are the easy half — F = qvB sin θ and F = BIL sin θ, largest across the field, zero along it, always sideways.

Faraday in one line

EMF = N × (flux change) ÷ (time) — the rate, times the turns. Double the turns, double the EMF; halve the rate, halve it. Flux itself induces nothing: a coil motionless in a strong magnet gives zero.

Nearly every induction stem is one of a small number of set-ups. Before anything else, name which term of Φ = BA cos θ the apparatus is changing.
Set-upTerm that changesWhat that tells you immediately
Loop dragged out of a uniform fieldarea in the field, Aan EMF only while an edge is crossing the boundary
Magnet falling through a coilfield through the coil, Btwo pulses of opposite sign, with a zero between them
Coil rotating between the polesorientation, θalternating EMF, largest edge-on, where the field skims across the face
Neighbouring circuit switched offfield through the loop, Ban EMF although nothing moves, lasting only while the current dies
Row three is the surprise: the coil generates most strongly edge-on, where flux is momentarily zero but changing fastest.

Moving fast is not the same as changing flux

A loop moving entirely inside a uniform field has constant flux and no EMF, however hard it is dragged: induction happens at the boundary. Nor need anything move — a loop beside a circuit switching off gets an EMF while its field dies.

Run any induction stem this way

1

Name which term of Φ = BA cos θ changes

θ is from the normal to the face: flux maximum face-on, zero edge-on. Only three things change it — B, the area in the field, or the orientation.

2

Growing or shrinking?

Ask whether flux that way is rising or falling. Everything downstream answers this.

3

The induced current opposes the CHANGE, not the field

Growing → the loop makes a field against it; shrinking → with it. Not against the existing field — half the wrong answers are that substitution. Right hand: thumb along the field the loop must make, fingers give the current.

4

Check the force

It fights what you are doing, so your work becomes the electrical energy. A coil helping the motion is a sign error.

figure unavailable: figure spec is not valid JSON
Two lobes of opposite sign: flux builds as the magnet arrives, dies as it leaves. Zero where it is level with the coil — maximum flux is momentarily unchanging. Taller and briefer leaving, same area.

Worked example

A square loop of side 0.20 m is pulled at 0.50 m/s out of a uniform 0.40 T field, perpendicular to the loop. What EMF appears as it leaves, and once fully outside?

Check yourself

A hand-cranked generator spins a 200-turn coil in a fixed magnetic field and produces a peak EMF of 12 V. The coil is rewound with 400 turns of the same size and shape, and the handle is then turned at half the previous rate. The new peak EMF is closest to:

Key takeaways

  • Φ = BA cos θ — only B, area, or angle can change it. Name which one first.
  • EMF = turns × RATE of flux change. Steady flux induces nothing.
  • Lenz: the current opposes the change, so the force fights the motion.
  • No change, no EMF — induction happens at the boundary.

Practise this with real GAMSAT-style questions

Free account: a timed diagnostic, an AI tutor that explains every answer, essay marking on the official rubric, and a plan built around your weak spots.

Start free
7 min read · Concept