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dave1368/cluster-09-thermal-exergy

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Cluster 9: Thermal Exergy & Macro-Thermodynamics

A neuro-symbolic system pairing exact classical efficiency limits ("Symetria Engine") with a trained neural network that predicts local entropy generation, exergy destruction, and cycle efficiency across a heat engine operating between a hot and cold reservoir, under LangGraph rollback/HITL supervision with two safety checks.

This is the final cluster in the series. Give it a hot and cold reservoir temperature; it computes the exact Carnot and Curzon-Ahlborn efficiency limits, runs a GPU network to predict how much useful work-potential ("exergy") is being destroyed at different points in the cycle, and checks the result against two physics safeguards before returning it.

How it works

  1. 1.Symetria Engine (exact): two classical efficiency limits for a heat engine running between temperatures Th (hot) and Tc (cold) — η_Carnot = 1 − Tc/Th (the absolute reversible upper bound, Carnot 1824) and η_CA = 1 − √(Tc/Th) (the efficiency a real engine actually achieves at maximum power output, Curzon & Ahlborn 1975).
  2. 2.GPU Exergy Field Network: a neural network that predicts entropy generation, exergy destruction, and cycle efficiency at any point between the two reservoirs, for any (Th, Tc) pair.
  3. 3.Physics safeguards:
  4. 4.Second Law check — entropy generation can never be negative.
  5. 5.Carnot-limit check — predicted efficiency can never exceed the reversible Carnot bound.
  6. 6.LangGraph orchestration — if either check fails, the pipeline rolls back and retries (bounded attempts) before surfacing a human-in-the-loop flag.

Validated against classical sources

Cluster 9's Master Specification cites Carnot (1824), Clausius (1865), Gouy (1889) & Stodola (1905), and Curzon & Ahlborn (1975). Each was independently re-derived in a fresh script and cross-checked against both the exact solver and the trained network — not read back from the project's own logs.

1. The two classical efficiency formulas, checked independently

Th (°C)Tc (°C)Carnot: solverCarnot: independentCurzon-Ahlborn: solverCurzon-Ahlborn: independent
600250.6585350.6585350.4156500.415650
10001000.7069080.7069080.4586200.458620
200−200.4649690.4649690.2685420.268542
1500−500.8741510.8741510.6452470.645247

Exact match at every point, as expected for closed-form formulas.

2. A structural fact, checked across the whole slider range: the real-engine limit never beats the reversible one

A real heat engine running at its maximum-power operating point (Curzon- Ahlborn) can never be more efficient than the theoretical reversible limit (Carnot) — that's not just true at a few sample points, it has to hold everywhere. Checked across 420 (Th, Tc) pairs spanning the full slider range: zero violations of ηCA ≤ ηCarnot.

3. Re-deriving the efficiency/entropy-generation identity from scratch

The exact identity linking cycle efficiency to entropy generation (η = η_Carnot − Tc·s_gen, where s_gen is entropy generated per unit of heat input) was re-derived independently here from the Clausius inequality and basic energy balance, not copied from the project's own code:

Starting from S_gen = Qc/Tc − Qh/Th ≥ 0 (Clausius), W = Qh − Qc, and η = W/Qh: substituting Qc = Qh·(1−η) gives s_gen = S_gen/Qh = (1−η)/Tc − 1/Th, which rearranges to η = η_Carnot − Tc·s_gen — matching the identity the project's own code uses. Plugging a chosen s_gen in, computing η, then working the Clausius formula backward from that η reproduces the same s_gen to 9 decimal places, confirming the identity is self-consistent, not just asserted.

4. Gouy-Stodola (1889/1905): exergy destruction, checked independently

Exergy destroyed = T₀ × entropy generated, where T₀ is the environment's reference temperature (298.15 K here). Recomputed with an independently typed-in T₀ rather than the code's own constant — matches exactly at every tested entropy-generation value.

5. Trained network vs. the exact identity, across several reservoir pairs

Th (°C)Tc (°C)Fraction of Carnot deficitEfficiency: predEfficiency: exact\err\
600250.10.59370.59270.0010
600250.50.32520.32930.0041
600250.90.06690.06590.0010
10001000.10.63540.63620.0008
10001000.50.35310.35350.0004
10001000.90.06910.07070.0016
200−200.10.41210.41850.0064
200−200.50.23510.23250.0026
200−200.90.04430.04650.0022

Errors stay small (under ~1% of the efficiency scale) across the whole tested range.

6. Two safety checks, two different stories

The Second Law check is structurally guaranteed to pass. The entropy-generation output is built using a mathematical function (Softplus) that can only ever produce zero or positive numbers, by construction — not something training could get wrong even if it tried. Confirmed by feeding the network deliberately broken (randomly scaled, sign-flipped) weights and checking the output anyway: minimum entropy generation across 20,000 points was exactly 0.0, never negative. This means the check can't tell a good model from a bad one, but it does guarantee this particular physical requirement is never violated.

The Carnot-limit check is a real, meaningful check — with one asymmetry worth knowing about. Unlike the Second Law check, this one genuinely can fail: feeding the network moderately scaled-up broken weights produced a mean efficiency of 1.89 (188.6%), and the check correctly caught it as exceeding the Carnot limit. But pushing the weights further (more extreme corruption) produced a wildly negative mean efficiency (as low as −22.8), and the check passed that too — it only checks whether efficiency is too high, not whether it's physically nonsensical in the other direction. In practice, the trained network's efficiency predictions stay well-behaved (see table above), so this asymmetry hasn't caused an actual wrong pass/fail in normal use — but it's worth knowing the check isn't a complete sanity test on its own.

Try it

Set a hot and cold reservoir temperature and run the pipeline. The app reports the exact Carnot and Curzon-Ahlborn limits, the total exergy destruction across the sampled field, the network's predicted efficiency, and whether both safety checks passed.

Limitations

  • —The Second Law check can't distinguish a good model from a bad one — see finding 6 above. Its only value is a structural guarantee, not a quality measure.
  • —The Carnot-limit check only catches efficiency being too high, not being nonsensically negative — see finding 6 above.
  • —This models the general thermodynamic identities of a heat engine, not a specific engine cycle (Rankine, Brayton, etc.) — the spatial field being sampled represents an abstract operating-point sweep, not a real engine's physical geometry.

Dependencies

  • —torch — GPU network inference
  • —langgraph — rollback/HITL orchestration state machine
  • —gradio — this interface
  • —wolframclient / neo4j are optional; both degrade gracefully to in-code fallbacks when absent (as here).