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## ERQ · 12 marks · Topics: E.3 Radioactive decay + B.1 Thermal energy transfers · Archetype: data_response
**Integration:** primary=E.3 Radioactive decay, secondary=B.1 Thermal energy transfers (strength: supporting)
**Stem.** A sealed stainless-steel capsule contains 8.0 × 10¹⁸ nuclei of cobalt-60 (half-life T₁/₂ = 5.27 yr), used as a low-power heat source in a laboratory calibration rig. Each β⁻ decay (followed by two γ photons) deposits, on average, 3.15 MeV of energy in the capsule walls and surrounding argon gas. The capsule sits inside a vacuum-jacketed enclosure of external surface area A_s = 0.045 m² and effective surface heat-transfer coefficient h = 1.8 W m⁻² K⁻¹ to a laboratory at 295 K. Students log the internal gas temperature T_gas and the outer-wall temperature T_wall monthly for 5 years; selected data are shown in the table below.
| t / yr | Activity A / 10¹⁰ Bq | T_gas / K | T_wall / K |
|---|---|---|---|
| 0.0 | 3.34 | 295 | 295 |
| 0.5 | 3.13 | 338 | 332 |
| 1.0 | 2.93 | 346 | 340 |
| 2.0 | 2.57 | 349 | 343 |
| 3.0 | 2.26 | 346 | 340 |
| 5.0 | 1.74 | 342 | 337 |
### Part (a) State and Define [2 marks] · AO1 · Topic: E.3
State the exponential law of radioactive decay in terms of the decay constant λ, and define the half-life of cobalt-60.
### Part (b)(i) Calculate [3 marks] · AO2 · Topic: E.3
Using T₁/₂ = 5.27 yr, calculate the decay constant λ (in s⁻¹) for cobalt-60, and verify that the initial activity A₀ of the sample is consistent with the t = 0 value in the table.
### Part (b)(ii) Determine [3 marks] · AO2 · Topic: E.3 + B.1
Determine the total thermal energy (in joules) released inside the capsule during the first half-life of the source.
### Part (c) Explain [2 marks] · AO3 · Topic: E.3 + B.1
The temperature data show that, after an initial rise, the gas temperature stabilises near ~348 K rather than continuing to climb as decay energy accumulates. Explain, using the concept of thermal equilibrium with the surroundings, why a steady temperature is reached, and identify the dominant mode of heat transfer from the outer wall to the laboratory.
### Part (d) Evaluate [2 marks] · AO3 · ASSUMPTIONS DISCRIMINATOR
A student models the capsule as a constant-power heat source over the full 5-year measurement window. Evaluate the validity of this constant-power assumption using the data in the table.
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## Mark Scheme
### Part (a) [2 marks]
- M1: Statement of decay law N = N₀ e^(−λt) OR equivalently A = A₀ e^(−λt) with symbols defined [no ECF]
- M2: Half-life defined as the time for the number of (cobalt-60) nuclei / activity to fall to half its initial value [no ECF]
### Part (b)(i) [3 marks] — Calculate
- M1: Convert T₁/₂ to seconds: 5.27 × 365.25 × 24 × 3600 = 1.66 × 10⁸ s [no ECF]
- M2: λ = ln 2 / T₁/₂ = 0.693 / 1.66 × 10⁸ = 4.17 × 10⁻⁹ s⁻¹ [ECF from M1]
- M3: A₀ = λN₀ = (4.17 × 10⁻⁹)(8.0 × 10¹⁸) = 3.34 × 10¹⁰ Bq, matches table value [ECF from M2]
### Part (b)(ii) [3 marks] — Determine
- M1: Mean activity over first half-life calculated as Ā = (A₀ − A₀/2)/ln 2 = A₀/(2 ln 2) = 2.41 × 10¹⁰ Bq, OR equivalently total decays = N₀/2 = 4.0 × 10¹⁸ [ECF from (b)(i)]
- M2: Convert energy per decay to SI: E_dec = 3.15 × 10⁶ × 1.60 × 10⁻¹⁹ = 5.04 × 10⁻¹³ J [no ECF]
- M3: Total thermal energy = (number of decays) × E_dec = 4.0 × 10¹⁸ × 5.04 × 10⁻¹³ ≈ 2.0 × 10⁶ J [ECF from M1, M2]
### Part (c) [2 marks] — Explain (causal chain per §4.4.1)
- M1: Heat is lost from the outer wall to the surroundings at a rate that increases with the wall–lab temperature difference (e.g. P_loss = hA_s ΔT), therefore as T_wall rises the loss rate grows until it equals the decay heating rate
- M2: At equilibrium, P_loss = P_decay, so T_gas stabilises; the dominant mode across the vacuum jacket / air gap to the laboratory is (free/natural) convection from the outer wall surface [accept radiation as co-dominant if justified]
### Part (d) [2 marks] — Evaluate (position + supporting + limiting per §4.4.1)
- M1: Position that the constant-power assumption is **invalid** over the full 5-year window, supported by data: activity falls from 3.34 → 1.74 × 10¹⁰ Bq (≈48% decrease), so decay power P = ĀE_dec falls by the same fraction; the observed peak in T_gas near t ≈ 2 yr followed by decline to 342 K is direct evidence of falling source power
- M2: Limiting/qualifying consideration that over **short intervals** (e.g. ≤ 1 yr) activity changes by only ~12%, so a piecewise- or instantaneous-constant-power treatment remains acceptable for short-term thermal modelling [accept: assumption acceptable only if t ≪ T₁/₂]
### Marker notes
- Alternative method accepted for (b)(ii): integrate P(t) = λN₀ E_dec e^(−λt) from 0 to T₁/₂ giving E = ½ N₀ E_dec = 2.02 × 10⁶ J — award M1 for setting up integral, M2 for SI energy conversion, M3 for correct evaluation.
- (b)(i) accept A₀ in range 3.3–3.4 × 10¹⁰ Bq.
- (c) accept radiation (Stefan–Boltzmann) as identified mechanism provided the temperature dependence (∝ T⁴) is referenced; conduction NOT accepted given vacuum jacket.
- (d) award M1 for any quantitative use of two table activity values OR for citing the T_gas peak-and-decline trend; award M2 for any valid restriction of the assumption's domain of validity (short Δt, or t ≪ T₁/₂, or ≤ one half-life with stated tolerance).
- ECF: candidates using λ or A₀ from (b)(i) in (b)(ii) receive full ECF credit.
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