## ERQ · 12 marks · Topics: C.2 Wave model + A.1 Kinematics · Archetype: experimental_analysis
**Integration:** primary=C.2 Wave model, secondary=A.1 Kinematics (strength: supporting)
**Stem.** A student investigates water waves in a rectangular ripple tank of length 0.80 m. A vertical dipper attached to a motor generates plane waves at one end of the tank; a stroboscope is used to "freeze" the wave pattern so that wavelengths can be measured on a scale beneath the tank. The student sets the motor frequency to f = 5.0 ± 0.1 Hz and, with the stroboscope adjusted, measures the distance across 6 successive crests as 0.150 ± 0.002 m. In a second procedure, the student instead measures the time taken for a single disturbance (made by tapping the water once) to travel the full 0.80 ± 0.01 m length of the tank, obtaining t = 5.4 ± 0.4 s. Finally, the student mounts the dipper on a small trolley moving with constant velocity 0.10 m s⁻¹ along the tank, in the same direction as the wave travel, and asks how the observed wavelength ahead of the trolley would change.
### Part (a) Define [2 marks] · AO1 · Topic: C.2 Wave model
Define (i) wavelength and (ii) frequency for a travelling wave.
### Part (b)(i) Calculate [3 marks] · AO2 · Topic: C.2 Wave model
Using the measurements from the stroboscope procedure, calculate the speed of the water waves in the tank.
### Part (b)(ii) Determine [2 marks] · AO2 · Topic: C.2 Wave model + A.1 Kinematics
Using the single-disturbance timing procedure, determine a second value for the wave speed.
### Part (c) Comment on [3 marks] · AO3 · Topic: C.2 Wave model
By propagating the relevant uncertainties, comment on whether the two values of wave speed obtained in (b)(i) and (b)(ii) are consistent.
### Part (d) Discuss [2 marks] · AO3 · ASSUMPTIONS DISCRIMINATOR · Topic: C.2 Wave model + A.1 Kinematics
With the dipper now moving on the trolley at 0.10 m s⁻¹, the student claims the relation v = fλ predicts that the wavelength ahead of the trolley becomes (v − v_source)/f. Discuss one assumption underlying this prediction whose breakdown in a real ripple tank could limit its validity.
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## Mark Scheme
### Part (a) [2 marks]
- M1: Wavelength = shortest distance between two points on the wave oscillating in phase / distance between successive crests [no ECF]
- M2: Frequency = number of complete oscillations (of a point in the medium / of the source) per unit time [no ECF]
### Part (b)(i) [3 marks] — Calculate
- M1: Recognises that 6 crests span 5 wavelengths, so λ = 0.150 / 5 = 0.030 m [no ECF]
- M2: Correct substitution into v = fλ = 5.0 × 0.030 [no ECF]
- M3: v = 0.15 m s⁻¹ (accept 0.150 m s⁻¹) [ECF from M1]
### Part (b)(ii) [2 marks] — Determine
- M1: Uses v = d/t with d = 0.80 m, t = 5.4 s [no ECF]
- M2: v = 0.148 ≈ 0.15 m s⁻¹ [ECF from M1]
### Part (c) [3 marks] — Comment on (evidence-tied interpretation)
- M1: Fractional uncertainty in v from (b)(i): Δv/v = Δλ/λ + Δf/f = 0.002/0.150 + 0.1/5.0 ≈ 0.013 + 0.020 = 0.033, giving v₁ = 0.15 ± 0.005 m s⁻¹ [ECF from (b)(i)]
- M2: Fractional uncertainty in v from (b)(ii): Δv/v = Δd/d + Δt/t = 0.01/0.80 + 0.4/5.4 ≈ 0.013 + 0.074 = 0.087, giving v₂ = 0.15 ± 0.013 m s⁻¹ [ECF from (b)(ii)]
- M3: Ranges (0.145–0.155) and (0.135–0.161) m s⁻¹ overlap, therefore the two measurements ARE consistent within experimental uncertainty [ECF from M1, M2]
### Part (d) [2 marks] — Discuss (assumption critique per §4.4.1)
- M1: Identifies an assumption — e.g. the wave speed v in water is independent of the source motion / the medium (water) is stationary in the lab frame / the trolley moves at strictly constant velocity / dispersion (frequency-dependence of v) is negligible / reflections from the far end do not interfere with the forward-travelling wave
- M2: Explains how its breakdown limits validity — e.g. shallow water waves are dispersive so a change in apparent wavelength would also change v, meaning (v − v_source)/f no longer gives the true observed λ; OR if the trolley accelerates over its short run, v_source in the formula is not well-defined kinematically; OR reflections superpose with outgoing waves so the "wavelength ahead" cannot be cleanly identified
### Marker notes
- Alternative method accepted for (b)(i): student may use λ from any consistent count of crest-to-crest intervals, provided 5 intervals are recognised between 6 crests.
- For (c), accept absolute-uncertainty addition method giving similar overlap conclusion; conclusion mark (M3) requires explicit reference to overlap of ranges.
- For (d), accept any one well-explained assumption from the list; do NOT award M2 without a physical mechanism linking the assumption to a quantitative or qualitative limitation. Mere restatement of the assumption ≠ M2.
- Numerical illustration for (d) (not required for marks): v_source·T = 0.10/5.0 = 0.020 m, predicted λ′ = 0.030 − 0.020 = 0.010 m.