AQA · A-Level · Physics
Course version: 7408 · Version from Sept 2016
Magnitude of induced emf = rate of change of flux linkage ∆Φ ε = N ∆t…
Full specification wording
Electromagnetic induction (A-level only): Magnitude of induced emf = rate of change of flux linkage ∆Φ ε = N ∆t Applications such as a straight conductor moving in a magnetic field.
The magnitude of an induced emf equals the rate of change of flux linkage, written ε = N ΔΦ/Δt, where N is the number of turns and ΔΦ/Δt is the rate of change of flux through one turn.
Checked against the AQA 7408 specification (opens in a new tab) on .
- Point 3 of 4
- 4 key terms
Study notes
From the checked teaching notes for this specification point.
The idea
The magnitude of an induced emf equals the rate of change of flux linkage, written ε = N ΔΦ/Δt, where N is the number of turns and ΔΦ/Δt is the rate of change of flux through one turn. For a straight conductor of length L moving with speed v perpendicular to a uniform magnetic field B, the emf is ε = BLv because the conductor sweeps area at a rate Lv and cuts flux at that rate. This applies to a rod sliding on rails, a falling conductor or an aircraft wing moving through the Earth’s field. The direction is found from Lenz’s law or the right-hand rule for a moving conductor. If the conductor moves parallel to the field, no flux is cut and the induced emf is zero.
What earns the marks
- The magnitude of the induced emf is the rate of change of flux linkage, ε = N ΔΦ/Δt, with ΔΦ measured in webers and Δt in seconds.
- For a straight conductor of length L moving at speed v perpendicular to a uniform field B, the induced emf is ε = BLv.
- The BLv result follows because the conductor sweeps area at rate Lv, so the rate of change of flux linkage is B × Lv for a single conductor.
- The direction of the induced emf or current is determined by Lenz’s law or by the right-hand rule for a moving conductor.
- If the conductor moves parallel to the magnetic field, it cuts no flux lines and the induced emf is zero.
- Applications include a rod sliding on conducting rails, a conductor falling through a magnetic field and a search coil moving through a field.
Common mistakes and how to put them right
Using ε = BLv when the conductor moves parallel to the field.
Put it right: Recognise that no flux is cut and the induced emf is zero.
Forgetting to include the number of turns N when a coil rather than a single conductor is moving.
Put it right: Use ε = N ΔΦ/Δt or multiply the single-conductor result by N where appropriate.
Mixing up the direction rule for a moving conductor with the direction rule for a current-carrying conductor in a field.
Put it right: Use the moving-conductor rule or Lenz’s law consistently.
Exam tips
- Identify the quantity changing with time before choosing between ε = N ΔΦ/Δt and ε = BLv.
- For a straight conductor, check that the velocity component is perpendicular to the field and use that component in ε = BLv.
- State the direction of the induced current separately from the magnitude calculation, using Lenz’s law or the moving-conductor rule.
Try the lesson
The start of the Electromagnetic induction (A-level only): Magnitude of induced emf = rate of change of flux linkage ∆Φ ε = N ∆t Applications such as a straight conductor moving in a magnetic field. lesson, made from checked teaching notes for this specification point.
Have a go first
A coil of 200 turns experiences a change in magnetic flux of 0.40 Wb in a time of 0.20 s. What is the magnitude of the average induced emf?
Listen
The magnitude of an induced emf equals the rate of change of flux linkage, written ε = N ΔΦ/Δt, where N is the number of turns and ΔΦ/Δt is the rate of change of flux through one turn. For a straight conductor of length L moving with speed v perpendicular to a uniform magnetic field B, the emf is ε = BLv because the conductor sweeps area at a rate Lv and cuts flux at that rate. This applies to a rod sliding on rails, a falling conductor or an aircraft wing moving through the Earth’s field. The direction is found from Lenz’s law or the right-hand rule for a moving conductor. If the conductor moves parallel to the field, no flux is cut and the induced emf is zero. A strong answer earns marks for these points. The magnitude of the induced emf is the rate of change of flux linkage, ε = N ΔΦ/Δt, with ΔΦ measured in webers and Δt in seconds. For a straight conductor of length L moving at speed v perpendicular to a uniform field B, the induced emf is ε = BLv. The BLv result follows because the conductor sweeps area at rate Lv, so the rate of change of flux linkage is B × Lv for a single conductor. The direction of the induced emf or current is determined by Lenz’s law or by the right-hand rule for a moving conductor. A common slip: Using ε = BLv when the conductor moves parallel to the field. Instead, recognise that no flux is cut and the induced emf is zero. Exam tip: Identify the quantity changing with time before choosing between ε = N ΔΦ/Δt and ε = BLv.
Key words
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Rate of change of flux linkage
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Motional emf
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Straight conductor in a magnetic field
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Direction of induced current
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See every definition
- Rate of change of flux linkage
- The magnitude of the induced emf equals this quantity, written ε = N ΔΦ/Δt, with ΔΦ measured in webers and Δt in seconds.
- Motional emf
- For a straight conductor of length L moving at speed v perpendicular to a uniform field B, the induced emf is ε = BLv.
- Straight conductor in a magnetic field
- The BLv result follows because the conductor sweeps area at rate Lv, so the rate of change of flux linkage is B × Lv for a single conductor.
- Direction of induced current
- This is determined by Lenz’s law or by the right-hand rule for a moving conductor.
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