```
## ERQ · 14 marks · Topics: D.4 Induction + B.5 Current and circuits · Archetype: data_response
**Integration:** primary=D.4 Induction, secondary=B.5 Current and circuits (strength: supporting)
**Stem.** A student investigates electromagnetic induction using a rectangular coil of N = 50 turns pulled horizontally at constant velocity v = 0.40 m s⁻¹ through a region of uniform magnetic field B = 0.25 T directed into the page. The coil has width w = 0.080 m (perpendicular to v and to B) and total resistance R = 1.5 Ω. A high-impedance datalogger records the EMF ε across the coil terminals as a function of time t as the coil enters, fully occupies, and then exits the field region. The recorded trace is shown below.
```
ε / V
0.40 ┤ ┌──────────┐
│ │ │
0.30 ┤ │ │
│ │ │
0.20 ┤ │ │
│ │ │
0.10 ┤ │ │
│ │ │
0.00 ┼──────┘ └──────────┐
│ │
-0.10 ┤ │
│ │
-0.20 ┤ │
│ │
-0.30 ┤ │
│ │
-0.40 ┤ └────────
└┬──────┬──────────┬──────────┬──────
0 0.20 0.60 0.80 t/s
```
The flat plateau of magnitude ε₀ = 0.40 V lasts from t = 0.20 s to t = 0.60 s during entry. The student also notes that the leading edge of the coil enters the field at t = 0.20 s.
### Part (a) Define [2 marks] · AO1 · Topic: D.4 Induction
Define *magnetic flux linkage* and state its SI unit.
### Part (b)(i) State [2 marks] · AO2 · Topic: D.4 Induction
State and explain why the recorded EMF is zero between t = 0 and t = 0.20 s, and again after the coil has fully entered the field.
### Part (b)(ii) Calculate [3 marks] · AO2 · Topic: D.4 Induction
Using the plateau value ε₀ = 0.40 V, calculate the length L of the coil in the direction of motion. (Note: the plateau ends when the trailing edge enters the field.)
### Part (c) Determine [3 marks] · AO2 · Topic: D.4 Induction
Determine the total electrical energy dissipated in the coil's resistance during the entry phase (0.20 s ≤ t ≤ 0.60 s).
### Part (d) Derive [2 marks] · AO2 · Topic: D.4 Induction + B.5 Current and circuits
The datalogger is now replaced with a low-resistance ammeter of internal resistance r = 0.50 Ω connected across the coil terminals. Derive an expression for the current I through the ammeter during the entry-phase plateau in terms of N, B, w, v, R and r, and evaluate it numerically.
### Part (e) Suggest [2 marks] · AO3 · ASSUMPTIONS DISCRIMINATOR
The student claims that the flat plateau in the EMF trace *proves* that the magnetic field B is spatially uniform throughout the field region. Suggest a way in which the field could in fact be non-uniform yet still produce the observed flat plateau.
---
## Mark Scheme
### Part (a) [2 marks]
- M1: Flux linkage is the product of the number of turns and the magnetic flux through one turn, NΦ (or N·B·A·cosθ) [no ECF]
- M2: SI unit is the weber (Wb) — accept V·s or T·m² [no ECF]
### Part (b)(i) [2 marks] — State and explain
- M1: Before t = 0.20 s the coil is outside the field, so flux linkage is zero / not changing ⟹ ε = 0 [no ECF]
- M2: Once fully inside the field, flux linkage is constant (maximum) so dΦ/dt = 0 ⟹ ε = 0 [no ECF]
### Part (b)(ii) [3 marks] — Calculate
- M1: Recognises that the duration of the plateau Δt = 0.60 − 0.20 = 0.40 s equals the time for the coil to be fully drawn into the field, so L = v·Δt [no ECF]
- M2: Correct substitution L = 0.40 × 0.40 [ECF from M1]
- M3: L = 0.16 m (accept 0.16 m to 2 sf) [ECF from M1, M2]
### Part (c) [3 marks] — Determine
- M1: Current during plateau I = ε₀ / R = 0.40 / 1.5 = 0.267 A (accept 0.27 A) [no ECF]
- M2: Power dissipated P = ε₀·I = 0.40 × 0.267 = 0.107 W (or equivalently I²R) [ECF from M1]
- M3: Energy E = P·Δt = 0.107 × 0.40 = 0.043 J (accept 0.042 – 0.043 J) [ECF from M1, M2]
### Part (d) [2 marks] — Derive (Topic 2 supporting role)
- M1: Identifies ε = N·B·w·v as the EMF source, with total series resistance R + r, giving I = N·B·w·v / (R + r) [no ECF]
- M2: Numerical evaluation: I = 0.40 / (1.5 + 0.50) = 0.20 A [ECF from M1]
### Part (e) [2 marks] — Suggest (proposal + warrant per §4.4.1)
- M1 (proposal): States a specific way in which B could be non-uniform yet compatible with a flat plateau — e.g. B varies spatially in the direction perpendicular to v (across the coil width w) but is independent of position along v; OR B varies along v but in a way that makes the line-integral B(x)·w constant as the leading edge sweeps; OR fringing exists at top/bottom of the field region symmetrically
- M2 (justification): Explicit physics warrant — the induced EMF depends only on the rate of flux sweeping ε = N·v·∫B·dy across the leading edge, so any variation that leaves the integrated flux per unit displacement constant produces the same plateau; transverse variation in B is averaged over the leading-edge length and does not appear in the time-trace [must logically link to M1]
### Marker notes
- Part (b)(ii): alternative method accepted — from ε₀ = N·B·w·v, verify that ε₀ is independent of L (used only to confirm plateau), then use plateau-duration argument; full marks if logic is equivalent.
- Part (c): accept calculation via I²·R·Δt directly (M1 current, M2 I²R, M3 ×Δt).
- Part (d): if student incorrectly omits r and writes I = NBwv/R = 0.267 A, award M1 only.
- Part (e): award 1 mark for a proposal without justification, OR a justification without an identifiable proposal; award 2 marks only when both components are present and logically linked. Accept any of:
- transverse non-uniformity (B = B(y) across width w) + averaging-over-leading-edge warrant
- B varies along v but ∫B dx remains linear in entry-displacement + flux-per-unit-time warrant
- symmetric fringing at field edges parallel to v + warrant that fringing does not contribute to dΦ/dt during entry
- Reject vague answers such as "the field could be slightly different" with no spatial specification (0 marks).
```