Generated ERQ

✓ passed B.4 Thermodynamics (HL) × A.3 Work, energy and power 14 marks HL 3 passes 120.23s $0.8085
## ERQ · 14 marks · Topics: B.4 Thermodynamics (HL) + A.3 Work, energy and power · Archetype: theory_application **Integration:** primary=B.4 Thermodynamics (HL), secondary=A.3 Work, energy and power (strength: supporting) **Stem.** A manufacturer demonstrates a small heat engine used to lift loads in a workshop. In each complete cycle the engine absorbs 8.5 kJ of thermal energy from a hot reservoir maintained at 450 K and rejects waste heat to a cold reservoir maintained at 300 K. The manufacturer states that the engine operates at 75% of the Carnot efficiency for these reservoir temperatures. The work output of the engine is delivered through a coupling to a hoist that lifts a 50 kg load vertically. Take g = 9.81 m s⁻² and assume the engine is in steady cyclic operation. ### Part (a) State [2 marks] · AO1 · Topic: B.4 Thermodynamics (HL) State the definition of the thermal efficiency of a heat engine, and write down the Carnot efficiency in terms of the hot and cold reservoir temperatures. ### Part (b)(i) Calculate [3 marks] · AO2 · Topic: B.4 Thermodynamics (HL) Calculate the maximum (Carnot) efficiency for the engine operating between the two reservoirs. Express your answer as a percentage. ### Part (b)(ii) Determine [2 marks] · AO2 · Topic: B.4 Thermodynamics (HL) Determine the actual thermal efficiency of the engine and the thermal energy, in kJ, rejected to the cold reservoir per cycle. ### Part (c) Calculate [3 marks] · AO2 · Topic: B.4 Thermodynamics (HL)+A.3 Work, energy and power Using the actual efficiency, calculate the useful work output per cycle and hence determine the maximum height to which the engine can raise the 50 kg load in one complete cycle, assuming the coupling to the hoist is ideal. ### Part (d) Evaluate [4 marks] · AO3 · ASSUMPTIONS DISCRIMINATOR A workshop technician measures that the load actually rises by only about 3.0 m per cycle, not the value predicted in part (c). Evaluate the manufacturer's claim that the engine delivers 75% of Carnot efficiency, with reference to specific irreversibilities and to the height calculated in (c). --- ## Mark Scheme ### Part (a) [2 marks] - M1: thermal efficiency η = W/Q_h (work output per cycle divided by thermal energy absorbed from hot reservoir) ✓ [no ECF] - M2: Carnot efficiency η_C = 1 − T_c/T_h (with T in kelvin) ✓ [no ECF] ### Part (b)(i) [3 marks] — Calculate - M1: identifies η_C = 1 − T_c/T_h with T_c = 300 K, T_h = 450 K ✓ [no ECF] - M2: η_C = 1 − 300/450 = 1 − 0.6667 = 0.3333 ✓ [ECF from (a)] - M3: η_C ≈ 33.3% (accept 33% or 0.33) ✓ [ECF from M2] ### Part (b)(ii) [2 marks] — Determine - M1: η_actual = 0.75 × 0.3333 = 0.250 (= 25.0%) ✓ [ECF from (b)(i)] - M2: Q_c = Q_h(1 − η_actual) = 8.5 × (1 − 0.250) = 6.375 ≈ 6.4 kJ ✓ [ECF from M1] ### Part (c) [3 marks] — Calculate (cross-topic with A.3) - M1: W = η_actual × Q_h = 0.250 × 8500 = 2125 J (≈ 2.13 kJ) ✓ [ECF from (b)(ii)] - M2: applies W = mgh ⇒ h = W/(mg) = 2125/(50 × 9.81) ✓ [ECF from M1] - M3: h ≈ 4.33 m (accept 4.3 m) ✓ [ECF from M1, M2] ### Part (d) [4 marks] — Evaluate (position + supporting + limiting per §4.4.1) - **M1 (POSITION):** clear judgement that the manufacturer's 75%-of-Carnot claim is optimistic / overstates real performance, since the measured h ≈ 3.0 m is significantly less than the predicted h ≈ 4.33 m from (c) ✓ - **M2 (SUPPORTING — internal irreversibility, quantified):** identifies an internal irreversibility (e.g. finite-temperature heat transfer across the reservoir boundary, turbulent/viscous losses in the working fluid, incomplete combustion or heat leakage through engine walls) AND links it to reduced W per cycle (e.g. heat leakage of ~0.6 kJ would reduce W from 2.13 kJ to ~1.5 kJ) ✓ - **M3 (SUPPORTING — external irreversibility, quantified causal chain):** identifies an external dissipation (e.g. friction in the coupling/hoist, air drag on the load) AND provides an explicit "X therefore Y" link: e.g. frictional losses of ~0.65 kJ in the coupling reduce useful lifting work to ~1.47 kJ, therefore h_real = 1470/(50 × 9.81) ≈ 3.0 m, matching observation ✓ [ECF from (c)] - **M4 (LIMITING / QUALIFICATION):** qualifies the judgement, e.g. the 75%-of-Carnot factor may already encapsulate some internal irreversibilities so the manufacturer's claim refers to the engine alone (not the hoist system), OR Carnot itself is an unattainable upper bound so any real engine must fall below it; hence the shortfall to 3.0 m may be largely attributable to external coupling losses rather than a false claim ✓ ### Marker notes - Alternative method accepted for (b)(ii): compute W first (W = 0.25 × 8.5 = 2.125 kJ) then Q_c = Q_h − W = 6.375 kJ. - Alternative for (c): direct chain h = (0.75 × (1 − 300/450) × 8500)/(50 × 9.81) — full marks if reasoning visible. - (d) accept any combination of two distinct irreversibilities for M2/M3 from: finite-ΔT heat transfer, friction (bearings, piston, hoist coupling), viscous/turbulent fluid losses, heat leakage to surroundings, incomplete heat absorption from hot reservoir, mechanical vibration losses. M3 requires a quantitative or semi-quantitative link to h (or W) — purely qualitative statements receive M2 credit only. - (d) M4 accept either direction of qualification (defending OR further critiquing the claim) provided reasoning is physics-based. - ECF applies throughout (b), (c), and (d) where downstream numerical values depend on earlier parts.