Audit a closed-cycle heat input before dividing for efficiency
A monatomic ideal gas executes a clockwise pressure-volume rectangle starting at 1 litre and 100 kPa. It heats at fixed volume to pressure 100a, expands at that pressure to b litres, cools at fixed volume to 100 kPa, then compresses back. A kPa litre equals one joule. This specifies quasistatic mechanical paths, not a realizable two-fixed-reservoir heat-transfer schedule.
Learning outcome: Retain a four-row table of delta U, work and signed heat. Add gas entropy changes, then explain what external temperature-contact evidence would be required to calculate total generation.
Starting recap
Review logarithmic integrals, equilibrium states, absolute temperature and the first-law work convention. State the domain and distinguish calibration data from unused validation.
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At a=3, b=2, work is 200 J, positive heat input 1050 J, rejected heat 850 J and efficiency 4/21≈0.190476. Energy closes 1050−850=200. The high-temperature corner has six times the low-temperature corner temperature.
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Which denominator gives the engine thermal efficiency?
Experiment
Retain a four-row table of delta U, work and signed heat. Add gas entropy changes, then explain what external temperature-contact evidence would be required to calculate total generation.
Separate positive heat input from cycle net heat
Worked teaching model · synthetic values · Clockwise rectangle: start (1 litre,100 kPa), heat at fixed volume, expand at high pressure, cool at fixed volume, compress at 100 kPa. Monatomic ideal gas U=3pV/2. Quasistatic mechanical paths; heat-contact implementation is unspecified, not a two-fixed-reservoir reversible engine.
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Ordered clockwise pressure-volume cycle
Graph axes rescale independently; read units and values, not screen angles. 1: start low-left; heat upward, expand right, cool down, compress left (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Ordered clockwise pressure-volume cycle
start low-left; heat upward, expand right, cool down, compress left
| volume (L) | pressure (kPa) |
|---|---|
| 1 | 100 |
| 1 | 300 |
| 2 | 300 |
| 2 | 100 |
| 1 | 100 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Net clockwise work | 200 | J |
| Positive heat input | 1050 | J |
| Rejected heat magnitude | 850 | J |
| Energy closure residual | 0 | J |
| Thermal efficiency | 0.1904762 | ratio |
| Maximum-to-minimum gas temperature ratio | 6 | ratio |
The enclosed work equals net heat, not total heat absorbed on the two heating legs.
Isochoric heat is 3 delta(pV)/2 and isobaric heat is 5p delta V/2. Sum positive legs separately from negative legs. The four gas entropy changes telescope to zero because the gas returns to its state; this does not establish zero entropy generation in unspecified external heat contacts. A range of gas temperatures is not itself a pair of fixed reservoirs.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
The enclosed work equals net heat, not total heat absorbed on the two heating legs.
Isochoric heat is 3 delta(pV)/2 and isobaric heat is 5p delta V/2. Sum positive legs separately from negative legs. The four gas entropy changes telescope to zero because the gas returns to its state; this does not establish zero entropy generation in unspecified external heat contacts. A range of gas temperatures is not itself a pair of fixed reservoirs.
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Which system boundary, reference path, constitutive law or independently calibrated record supports this entropy inference?
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