exam bank

Electromagnetism

One question unlocks the whole topic: does your system have a battery? That single decision splits every electromagnetism question into two distinct paths — a current creating a magnetic field, or a changing field inducing a current.

Electromagnetism
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⊗  Electromagnetism
Does the system have a battery?
YES
NO
YES — Battery present Current flows → creates a magnetic field
1
Cause
Current will flow
The battery maintains a potential difference that drives a continuous current through the conductor.
2
Effect
Creates a magnetic field
Every current-carrying conductor is surrounded by a magnetic field. The shape of that field depends entirely on the shape of the conductor. Choose below.
Choose the conductor shape
01 Single Straight Wire

The magnetic field forms concentric circles centred on the wire. The field is strongest close to the wire and weakens with distance — it never stops, it just keeps spreading out.

Right Hand Rule Point your right thumb in the direction the current flows. Your fingers curl in the direction of the magnetic field around the wire.
DOT (•) Current toward you — out of page
×
CROSS (×) Current away from you — into page
Exam tip: parallel wires Two parallel wires carrying current in the same direction attract each other (fields reinforce between them). Opposite directions → repel.
02 Current Loop

A single loop creates field lines that pass through the centre and bow outward on both sides — identical in shape to the field of a very flat bar magnet. The two faces of the loop behave like poles.

Right Hand Rule for a loop Curl your right-hand fingers in the direction the current flows around the loop. Your thumb points toward the North face (the face the field exits from).
Face rule (shortcut) Look directly at one face of the loop.
• Current flows anticlockwise → you're looking at the North pole.
• Current flows clockwise → you're looking at the South pole.
03 Solenoid (coil of wire)

A solenoid stacks many loops in a row, creating a uniform magnetic field inside its core. Outside the solenoid, the field pattern is identical to a bar magnet — with a North and South pole at the two ends.

Right Hand Rule for a solenoid Curl your right-hand fingers in the direction the current flows around the coils. Your thumb points to the North pole end.
Face rule (same as loop) Look at one end of the solenoid directly.
• Current flows anticlockwise → that end is the North pole.
• Current flows clockwise → that end is the South pole.

This also works in reverse: if you know the pole, you immediately know the current direction. The more turns (N) and the greater the current, the stronger the field.
NO — No battery Move a magnet → induces a current
1
Cause
Move a magnet near the conductor
No battery means no ready-made current. Instead, moving a magnet near a conductor changes the magnetic flux through it — and that change is what drives the current.
The three laws you need
Magnetic Flux
How much of the field passes through the surface. θ is the angle between the field and the normal to the surface.
\[\Phi = BA\cos\theta\]
Faraday's Law
The induced EMF is proportional to the rate of change of flux. More turns (N) = more EMF. Faster change = more EMF.
\[\varepsilon = -N\frac{\Delta\Phi}{\Delta t}\]
Lenz's Law
The induced current opposes the change in flux that caused it. The conductor always fights back against whatever is happening to it.
Memory trick The conductor is stubborn. Flux increasing? It tries to reduce it. Flux decreasing? It tries to maintain it. Always opposing.
2
Effect
An EMF is induced → current flows
The changing flux produces an EMF (Faraday), which drives a current. The direction of that current is determined by Lenz's law. Choose the conductor shape below.
Choose the conductor shape
01 Flat Loop (electromagnetic induction)

As the magnet moves toward the loop, the flux through it increases. By Lenz's law, the induced current creates a field that opposes that increase — the near face of the loop becomes a North pole, pushing back against the approaching magnet.

Step-by-step method 1. Identify which pole is approaching and in which direction.
2. Decide: is flux increasing or decreasing?
3. Lenz: induced B-field opposes the change.
4. The exam tells you which face to view from.
5. If induced B points toward you → anticlockwise current. Away → clockwise.
Magnet moving away Flux decreases → induced current tries to maintain flux → near face becomes a South pole, attracting the retreating magnet. The conductor always resists.
02 Solenoid (electromagnetic induction)

When the magnet moves into the solenoid, flux increases. The solenoid induces a current whose field opposes the entry — the near end becomes a North pole, repelling the incoming North pole of the magnet.

Lenz's Law applied to a solenoid • Magnet entering (N first) → near end = N (repels) → current anticlockwise viewed from that end.
• Magnet exiting (N first) → near end = S (attracts, resisting exit) → current reverses.
• The solenoid always opposes whatever the magnet is doing.
Finding current direction from the pole Once Lenz's law tells you which end is N or S, apply the face rule in reverse: North end = anticlockwise current on that face. Then trace the current through the external circuit to the galvanometer.
\[\varepsilon = -N\frac{\Delta\Phi}{\Delta t} \qquad \Phi = BA\cos\theta\]
The solenoid acts like a battery It has an induced EMF \(\varepsilon\) that drives a current through the external circuit. The faster the magnet moves, the greater the EMF — and the greater the deflection on the galvanometer.

Quick Reference

All five scenarios at a glance.

Scenario Battery? What happens Key rule Formula
Straight wire YES Concentric circular field around wire RHR — thumb = I, fingers = B
Current loop YES Field through centre; faces are N/S poles Face rule — anticlockwise = N
Solenoid (battery) YES Uniform field inside; bar-magnet field outside RHR + face rule
Flat loop (induction) NO Changing flux induces current in loop Lenz + face rule \(\varepsilon = -N\dfrac{\Delta\Phi}{\Delta t}\)
Solenoid (induction) NO Moving magnet induces EMF and current Lenz + face rule + RHR \(\varepsilon = -N\dfrac{\Delta\Phi}{\Delta t}\)
Magnetic flux Amount of B-field through a surface θ = angle between B and surface normal \(\Phi = BA\cos\theta\)
YES