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NotesPhysics HLTopic 4.4
Unit 4 · Fields · Topic 4.4

IB Physics HL — Induction (HL)

Topic 4.4 of IB Physics covers Induction (HL), which is part of Unit 4: Fields. Students explore key concepts including Principles of electromagnetic induction, Applications of electromagnetic induction. A strong understanding of induction (hl) is essential for IB Physics HL exams and builds the foundation for connected topics across the syllabus.

Higher Level students should use this topic hub as a map: start with the shared sub-topics, then follow the HL-only extensions and exam-skill links where this topic asks for deeper analysis.

Exam technique guidePractice questions

Key concepts in Induction (HL)

Key Idea: Wave a magnet through a coil and a needle flicks — no battery anywhere. That single idea — a changing magnetic flux induces a voltage (emf), Faraday's law — runs every generator and transformer on the grid. Lenz's law fixes the direction (the induced effect always opposes the change, conserving energy). It is HL only (D.4).

📐 The formulas you're given

Φ=BAcos⁡θε=−NΔΦΔtε=BvL\Phi = BA\cos\theta \qquad \varepsilon = -N\frac{\Delta\Phi}{\Delta t} \qquad \varepsilon = BvLΦ=BAcosθε=−NΔtΔΦ​ε=BvL
Φ\PhiΦ
magnetic flux (Wb); θ is between B and the NORMAL to the area
ε\varepsilonε
induced emf (V); the minus sign is Lenz's law
ε=BvL\varepsilon = BvLε=BvL
motional emf of a rod length L moving at v through field B
ε=BANωsin⁡(ωt)Irms=I02εpεs=NpNs=IsIp\varepsilon = BAN\omega\sin(\omega t) \qquad I_\text{rms} = \frac{I_0}{\sqrt{2}} \qquad \frac{\varepsilon_p}{\varepsilon_s} = \frac{N_p}{N_s} = \frac{I_s}{I_p}ε=BANωsin(ωt)Irms​=2​I0​​εs​εp​​=Ns​Np​​=Ip​Is​​
BANωBAN\omegaBANω
peak emf ε₀ of a coil (N turns, area A) rotating at ω
IrmsI_\text{rms}Irms​
rms current — the equivalent DC for the same heating
Np/NsN_p/N_sNp​/Ns​
transformer turns ratio (ideal: power is conserved)

✏️ IB-style worked examples (one per micro)

IB-style questionDetermine[2 marks]

The magnetic flux through a 50-turn coil falls steadily from 0.20 Wb to 0 in 0.10 s. Determine the magnitude of the induced emf.

🔒 Model answer plan

See the mark-by-mark plan — for / against / judgement, with marking guidance — in study mode.

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IB-style questionDetermine[2 marks]

A step-down transformer has 1000 primary turns and 50 secondary turns, with 230 V across the primary. Determine the secondary voltage.

🔒 Model answer plan

See the mark-by-mark plan — for / against / judgement, with marking guidance — in study mode.

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IB-style questionDetermine[2 marks]

A mains supply has a peak voltage of 325 V. Determine its rms voltage.

🔒 Model answer plan

See the mark-by-mark plan — for / against / judgement, with marking guidance — in study mode.

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Important: 1. Flux uses cos θ to the normal of the area — when B is along the plane of the coil, the flux is zero, not maximum. 2. The minus sign in Faraday's law is Lenz's law (opposition = energy conservation), not an arithmetic error. 3. Don't confuse rms and peak — divide the peak by √2. 4. It is the rate of change of flux that matters — a large but steady flux induces no emf.

Tap each card to reveal the answer.

What does magnetic flux depend on? Φ = BA cos θ — the field B, the area A, and the angle θ between B and the normal to the area.

State Faraday's law. The induced emf equals the rate of change of flux linkage: ε = −N ΔΦ/Δt.

State Lenz's law. The induced current opposes the change that caused it — a consequence of energy conservation (the minus sign).

Motional emf of a 0.40 m rod at 3.0 m/s in a 0.50 T field? 0.60 V — ε = BvL = 0.50 × 3.0 × 0.40.

Why are rms values used for AC? They give the equivalent DC that delivers the same average power (heating).

What does an ideal transformer conserve? Power — so stepping voltage up steps current down (and vice versa).

Exam tips

  • Always measure the flux angle to the NORMAL of the area, not to the surface.
  • Quote the minus sign as Lenz's law; it is direction, not a negative emf.
  • Divide a peak value by √2 to get rms (and ×√2 to go back).
  • Only a CHANGING flux induces an emf — emphasise 'rate of change'.
  • For transformers, use the turns ratio and remember power is conserved (ideal).

What you'll learn in Topic 4.4

  • 4.4.1 Principles of electromagnetic induction
  • 4.4.2 Applications of electromagnetic induction
Suggested study order: Read the notes for each sub-topic below → test yourself with flashcards → attempt practice questions → review exam technique.

Study resources — 4.4 Induction (HL)

4.4.1

Principles of electromagnetic induction

Notes
4.4.2

Applications of electromagnetic induction

Notes

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Topic 4.4 Induction (HL) forms a core part of Unit 4: Fields in IB Physics HL. Mastering these concepts will strengthen your understanding of connected topics across the syllabus and prepare you for exam questions that require analysis, evaluation, and real-world application.

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