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D.4.1 Induced Emf — IB Physics HL Revision Notes & Topical Questions

5 min read 8 parts Lesson 35 of 39 1 quiz

📚 IB Physics HL Hub / Topical Revision
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Lesson summary

D.4.1 Induced Emf — IB PHYSICS HL notes: Explain how an e.m.f. is induced when a conductor cuts magnetic field lines and use ε = BLv.Meaning — an e.m.f.

  • Formal definition
  • Force on electrons
  • Charge separation
  • Closed circuit
  • Larger e.m.f
  • Electromagnetic induction

Section 1 of 8Electromagnetic induction

Meaning
  • Meaning an e.m.f. is induced due to relative movement between a conductor and a magnetic field
Ways
  • Ways a conductor moves relative to the field or the field varies relative to a conductor
Formal definition
  • Formal definition the process in which an e.m.f. or current is induced in a closed circuit due to changes in magnetic flux

Section 2 of 8How the e.m.f. arises

Force on electrons
  • Force on electrons free electrons in a conductor that cuts field lines experience a magnetic force
Charge separation
  • Charge separation work is done as charges move to the ends of the conductor
Energy
  • Energy mechanical work is transferred to the charges as electric potential energy
Result
  • Result a potential difference exists between the ends, which is the induced e.m.f.
Definition
  • Definition induced e.m.f. is the work done per unit charge separating the charges to the ends of the conductor
Closed circuit
  • Closed circuit an induced current can flow

Section 3 of 8Moving straight conductor

Condition
  • Condition the conductor must be in a perpendicular field so it cuts the field lines
Circuit
  • Circuit the rest of the circuit lies outside the field so the e.m.f. is induced across the conductor in the field only
Equation
  • ε = BLv
Symbols
  • ε in V, B in T, L the length in the field in m and v the speed in m s−1
Larger ε
  • Larger ε longer conductor, stronger field or faster cutting of field lines
Coil
  • ε = BLvN for N turns

Section 4 of 8Experiment 1: magnet and coil

1
Connect the coil to a sensitive voltmeter.
2
Hold the magnet still inside or outside the coil and the reading is zero because the flux does not change.
3
Move the magnet into the coil and a momentary reading appears as the flux changes.
4
Withdraw the magnet and the reading is in the opposite direction.
5
Move the magnet faster and the reading is larger because the rate of change of flux is greater.
  • Larger e.m.f.
    • faster movement, more turns on the coil or a stronger magnet

Section 5 of 8Experiment 2: wire between magnets

1
Connect a long wire to a voltmeter, with no current in the wire to begin with.
2
Hold the wire still and the reading is zero.
3
Move the wire between the magnets and an e.m.f. is induced as it cuts the field lines.
4
Move the wire out and the e.m.f. is in the opposite direction.
  • Larger e.m.f.
    • a longer wire, faster movement or stronger magnets

Section 6 of 8More from the specification

1Faraday's Law of Electromagnetic Induction
  • Faraday's law states that induced electromotive force (voltage) in a circuit is directly proportional to the rate of change of magnetic flux linkage (ε = -N·ΔΦ/Δt),
    What the symbols mean: ε = induced e.m.f. (V) · N = number of turns · ΔΦ = change of flux (Wb) · Δt = time taken (s); the minus sign is Lenz’s law
  • where magnetic flux Φ = B·A cos θ.
2AC Generation and Flux Angle
  • In an alternating current generator, a coil rotating with angular frequency ω in a magnetic field of flux density B sweeps through angle θ = ωt;
    • induced voltage reaches its maximum value when the plane of the coil is parallel to the magnetic field.
3Transformer Mutual Induction
  • In a step-up or step-down transformer, an alternating voltage applied to the primary winding creates an alternating magnetic flux in the core that induces an alternating output emf across the secondary coil.
4Constant speed
  • Speed that does not change.
5Electromagnetic induction
  • Production of an e.m.f. by relative movement of a conductor and a magnetic field.
6Induction
  • Charging an object without touching it, giving it the opposite sign to the charged object.
7Density
  • Mass per unit volume.
8Frequency
  • Revolutions per second, f = 1/T.
    What the symbols mean: T = period, the time for one complete wave (s) · f = frequency (Hz)
9Primary
  • Input coil.
10Secondary
  • Output coil.
11Angular speed
  • Magnitude of the angular velocity.
12Mutual induction
  • Induction of an e.m.f. in one circuit by a change of current in a neighbouring circuit.
13Alternating current
  • Current that continually reverses direction.
14Φ = BA
What the symbols mean: Φ = magnetic flux (Wb) · B = magnetic flux density (T) · A = area at right angles to the field (m2)

Section 7 of 8Key terms

TermMeaning
Electromagnetic inductionThe induction of an e.m.f. or current in a closed circuit due to changes in magnetic flux.
Induced e.m.f.The work done per unit charge in separating charges to the ends of a conductor.
ε = BLvThe e.m.f. induced in a conductor of length L moving at speed v perpendicular to a field B.
Flux cuttingThe movement of a conductor across magnetic field lines.

Section 8 of 8Exam technique

1
Saying an e.m.f. is induced in a stationary conductor in a steady field — the flux must change.
2
Putting the whole circuit in the field — only the moving conductor in the field gives the e.m.f.
3
Taking L as the whole wire length rather than the part inside the field.
4
Forgetting that reversing the motion reverses the induced e.m.f.

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