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AP · AP C:E&M · extended response

Induced current opposes the change, not the field

AP Physics C: Electricity and Magnetism · Original GioPhysics question with a detailed, mark-by-mark answer guide.

Demand
discriminating
Marks
6
Topics
1
Answer
Complete
Explore the question data

Applied field through the coil

Supplied question data. Read the labelled axes and use the observations to test the physical model.

Vertical axis (y): Magnetic field / T

Applied field through the coilSupplied question data. Read the labelled axes and use the observations to test the physical model. Horizontal axis: Time / s. Vertical axis: Magnetic field / T. Exact values are available in the data table below.00.10.20.30.400.1750.350.5250.7xy

Horizontal axis (x): Time / s

Reading 1Time / s: 0Magnetic field / T: 0
Read the exact data as a table
Applied field through the coil — supplied values
Time / sMagnetic field / T
00
0.20.4
0.50.4
0.70

These are the supplied values, not a worked answer. Lines join the supplied values; they are not a fitted model.

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extended response6 marks

A 100-turn closed coil of area 0.010 m² and resistance 5.0 Ω has its normal parallel to a uniform magnetic field. The field changes linearly through the supplied points. Positive flux is defined along the coil normal; neglect self-inductance for the current calculation. Supplied data (Time / s; Magnetic field / T): (0, 0), (0.2, 0.4), (0.5, 0.4), (0.7, 0).

  1. (a)

    Calculate the signed induced emf and current during each interval, using ε = −N dΦ/dt.

    3 marks
  2. (b)

    Find total resistive energy dissipated and explain the energy source and current direction during the decreasing-field interval.

    3 marks
Ready to self-mark?Reveal the detailed answer guide
Answer overview(a) 0–0.2 s: ε = −2.0 V, I = −0.40 A; 0.2–0.5 s: zero; 0.5–0.7 s: ε = +2.0 V, I = +0.40 A. (b) Total heating = 0.32 J; the external apparatus changing the field supplies the energy.
01

(a)

3 marks

Calculate the signed induced emf and current during each interval, using ε = −N dΦ/dt.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    With the field normal to the coil, flux per turn is Φ = BA and flux linkage is NBA.

  2. 2

    The initial field gradient is +2.0 T s⁻¹, so ε = −100(0.010)(2.0) = −2.0 V and I = ε/R = −0.40 A.

  3. 3

    Constant field gives zero flux-change emf. The final gradient is −2.0 T s⁻¹, reversing both emf and current to +2.0 V and +0.40 A.

02

(b)

3 marks

Find total resistive energy dissipated and explain the energy source and current direction during the decreasing-field interval.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    During each 0.20 s ramp, I²Rt = (0.40)²(5.0)(0.20) = 0.16 J; total heating is 0.32 J.

  2. 2

    When the applied field decreases, the induced current creates a field in the original positive direction, opposing the decrease rather than always opposing the existing field.

  3. 3

    Lenz's law gives a reaction opposing the flux change. The apparatus maintaining that change must supply energy that is dissipated in the coil; induction is not a free source of energy.

Complete marking guidance

Use these worked steps alongside the part-by-part answers. They explain the method and mark allocation; they do not add extra marks.

  1. With the field normal to the coil, flux per turn is Φ = BA and flux linkage is NBA.
  2. The initial field gradient is +2.0 T s⁻¹, so ε = −100(0.010)(2.0) = −2.0 V and I = ε/R = −0.40 A.
  3. Constant field gives zero flux-change emf. The final gradient is −2.0 T s⁻¹, reversing both emf and current to +2.0 V and +0.40 A.
  4. During each 0.20 s ramp, I²Rt = (0.40)²(5.0)(0.20) = 0.16 J; total heating is 0.32 J.
  5. When the applied field decreases, the induced current creates a field in the original positive direction, opposing the decrease rather than always opposing the existing field.
  6. Lenz's law gives a reaction opposing the flux change. The apparatus maintaining that change must supply energy that is dissipated in the coil; induction is not a free source of energy.

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