Electromagnetic Induction: MDCAT Notes and MCQs
Faraday's law
The emf induced in a circuit is directly proportional to the rate of change of magnetic flux through it: ε = −N ΔΦ/Δt. Flux can be changed by moving a magnet, changing current in a nearby coil, rotating a coil, or changing area. Motional emf of a rod: ε = BLv.
Lenz's law
- The direction of the induced current is such that it opposes the change in flux that produces it (the minus sign in Faraday's law).
- Consequence of conservation of energy: work must be done against the opposing force; that work appears as electrical energy. If the induced current aided the change, energy would be created from nothing.
- Example: N-pole approaching a coil → near face becomes N (repels); receding → near face becomes S (attracts).
Transformer
- Construction: two coils (primary and secondary) wound on a laminated soft-iron core. Works on mutual induction — needs AC (changing flux); does not work on steady DC.
- Vs/Vp = Ns/Np = Ip/Is (ideal: VpIp = VsIs). Frequency is unchanged.
- Step-up: Ns > Np → voltage ↑, current ↓. Step-down: Ns < Np → voltage ↓, current ↑.
- Losses: eddy currents (reduced by laminating the core), hysteresis (soft iron), copper (I²R) losses (thick wires), flux leakage. Efficiency of large transformers ≈ 95–99%.
Power transmission
Power is stepped up to very high voltage (e.g. 132–500 kV) at the power station so that current is small; line loss P = I²R is greatly reduced. Step-down transformers near homes reduce voltage to 220 V for safe use.
PMDC learning outcomes for this unit
- Induction & transformers: 11.1 State Faraday's law of electromagnetic induction.
- Induction & transformers: 11.2 Account for Lenz's law to predict the direction of an induced current and relate it to conservation of energy.
- Induction & transformers: 11.3 Describe the construction of a transformer and explain how it works.
- Induction & transformers: 11.4 Describe how step-up and step-down transformers can be used to ensure efficient transfer of electricity along cables.