Revisiting Endo-reversible Carnot engine: Extending the Yvon engine
Pith reviewed 2026-05-23 07:16 UTC · model grok-4.3
The pith
Extending the Yvon engine shows it is equivalent to the Curzon-Ahlborn engine as steady-state and cyclic forms of the endo-reversible Carnot heat engine.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The extended Yvon engine and the CA engine represent the steady-state and cyclic forms of the endo-reversible Carnot heat engine respectively and are equivalent.
What carries the argument
The extension of the Yvon engine that removes its original special-setup limitations and permits direct equivalence proof with the CA engine.
Load-bearing premise
Extending the Yvon engine's special setup produces a model with exactly the same generality as the CA engine without adding hidden constraints.
What would settle it
A calculation of efficiency at maximum power for the extended Yvon engine that yields a different numerical result from the CA engine under matching conditions.
Figures
read the original abstract
A famous paper [Am. J. Phys. 43, 22 (1975)] unveiled the efficiency at maximum power (EMP) of the endo-reversible Carnot heat engine, now commonly referred to as the Curzon-Ahlborn (CA) engine, pioneering finite-time thermodynamics. Historically, despite the significance of the CA engine, similar findings had emerged at an earlier time, such as the Yvon engine proposed by J. Yvon in 1955 sharing the exact same EMP. However, the special setup of the Yvon engine has circumscribed its broader influence. This paper extends the Yvon engine model to achieve a level of generality comparable to that of the CA engine. A rigorous comparison reveals that the extended Yvon engine and CA engine represent the steady-state and cyclic forms of the endo-reversible Carnot heat engine, respectively, and are equivalent. Our work provides a pedagogical example for the teaching of thermodynamics and engineering thermodynamics, given that the simple and lucid derivation of the extended Yvon engine helps students initiate their understanding of non-equilibrium thermodynamics.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript extends the 1955 Yvon engine to a more general form comparable to the Curzon-Ahlborn (CA) engine. It claims that the extended Yvon model (steady-state) and the CA model (cyclic) are equivalent representations of the endo-reversible Carnot heat engine under identical linear heat-transfer laws, both recovering the same algebraic expression for efficiency at maximum power (EMP). The work presents an explicit, parameter-free derivation of the extended Yvon engine followed by side-by-side comparison, positioning the result as a pedagogical example for finite-time thermodynamics.
Significance. If the equivalence holds, the paper supplies a clear, simple derivation that can serve as an entry point for students learning non-equilibrium thermodynamics. The explicit parameter-free derivation and direct comparison of EMP expressions are strengths. The stress-test concern about hidden constraints from the extension does not appear to land, as the mapping preserves generality without additional restrictions on timing or coupling.
minor comments (2)
- [Abstract] Abstract: the phrase 'rigorous comparison' would be more accessible if it briefly indicated the main steps (e.g., the form of the extended heat-transfer law or the EMP derivation) rather than leaving the reader to infer them from the full text.
- [Introduction] The introduction would benefit from an explicit citation to the original 1955 Yvon reference when first describing the special setup, to strengthen the historical framing.
Simulated Author's Rebuttal
We thank the referee for the positive evaluation of our manuscript and the recommendation for minor revision. The report highlights the pedagogical value of the explicit derivation and the equivalence between the extended Yvon engine and the Curzon-Ahlborn engine. No specific major comments were listed under the MAJOR COMMENTS section.
Circularity Check
No significant circularity detected
full rationale
The paper's derivation begins from the 1955 Yvon setup, performs an explicit algebraic extension to match the generality of the 1975 CA model, and then compares the resulting EMP expressions side-by-side. Both the extension and the equivalence proof are parameter-free, use only the stated linear heat-transfer law, and do not invoke self-citations or fitted inputs for the central claim. The cited historical works are external and predate the present authors. No step reduces by construction to its own inputs; the argument remains self-contained against the external benchmarks of the two classic models.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Endo-reversible Carnot engine assumes internal processes are reversible while external heat transfers occur in finite time.
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel; Jcost_pos_of_ne_one matches?
matchesMATCHES: this paper passage directly uses, restates, or depends on the cited Recognition theorem or module.
P = ΓhΓc Th/(Γh+Γc) (1 + Tc/Th - θc/θh - Tc/Th · θh/θc) ≤ ... (1 - sqrt(Tc/Th))^2 achieved at θc/θh = sqrt(Tc/Th)
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IndisputableMonolith/Foundation/Cost.leanJcost_convexity; interactionDefect_RCLCombiner echoes?
echoesECHOES: this paper passage has the same mathematical shape or conceptual pattern as the Recognition theorem, but is not a direct formal dependency.
AM-GM inequality applied to obtain maximum power when Tm = sqrt(Th Tc)
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
F. L. Curzon and B. Ahlborn, Efficiency of a carnot engine at maximum power output, Am. J. Phys. 43, 22 (1975)
work page 1975
-
[2]
B. Andresen, Current trends in finite-time thermodynamics, Angewandte Chemie International Edition 50, 2690 (2011)
work page 2011
-
[3]
Tu, Recent advance on the efficiency at maximum power of heat engines, Chin
Z.-C. Tu, Recent advance on the efficiency at maximum power of heat engines, Chin. Phys. B 21, 020513 (2012)
work page 2012
-
[4]
H. S. Leff, Reversible and irreversible heat engine and refriger- ator cycles, Am. J. Phys. 86, 344 (2018)
work page 2018
-
[5]
Bejan, Models of power plants that generate minimum en- tropy while operating at maximum power, Am
A. Bejan, Models of power plants that generate minimum en- tropy while operating at maximum power, Am. J. Phys. 64, 1054 (1996)
work page 1996
-
[6]
M. Moreau and Y . Pomeau, Carnot principle and its generaliza- tions: A very short story of a long journey, Eur. Phys. J. Spec. Top. 224, 769 (2015)
work page 2015
-
[7]
H. Ouerdane, Y . Apertet, C. Goupil, and Ph. Lecoeur, Continu- ity and boundary conditions in thermodynamics: From carnot’s efficiency to efficiencies at maximum power, Eur. Phys. J. Spec. Top. 224, 839 (2015)
work page 2015
-
[8]
J. Yvon, Saclay Reactor: Acquired Knowledge by Two Years Experience in Heat Transfer Using Compressed Gas , Tech. Rep. (CEA Saclay, France, 1955)
work page 1955
-
[9]
Chambadal, Les centrales nucléaires (Armand Colin, Paris, 1957)
P. Chambadal, Les centrales nucléaires (Armand Colin, Paris, 1957)
work page 1957
-
[10]
I. I. Novikov, Efficiency of an atomic power generating instal- lation, The Soviet Journal of Atomic Energy 3, 1269 (1957)
work page 1957
-
[11]
L. Chen and Z. Yan, The effect of heat-transfer law on per- formance of a two-heat-source endoreversible cycle, J. Chem. Phys. 90, 3740 (1989)
work page 1989
-
[12]
Tu, Abstract models for heat engines, Front
Z.-C. Tu, Abstract models for heat engines, Front. Phys. 16, 33202 (2021)
work page 2021
-
[13]
Finite-time thermodynamics: A journey beginning with optimizing heat engines
Y .-H. Ma and X.-H. Zhao, Finite-time thermodynamics: A journey beginning with optimizing heat engines, arXiv preprint arXiv:2411.03853 10.48550/arXiv.2411.03853 (2024)
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2411.03853 2024
-
[14]
M. H. Rubin, Optimal configuration of a class of irreversible heat engines. i, Phys. Rev. A 19, 1272 (1979)
work page 1979
-
[15]
V . Holubec and A. Ryabov, Efficiency at and near maximum power of low-dissipation heat engines, Phys. Rev. E92, 052125 (2015)
work page 2015
-
[16]
N. Shiraishi, K. Saito, and H. Tasaki, Universal trade-off rela- tion between power and efficiency for heat engines, Phys. Rev. Lett. 117, 190601 (2016)
work page 2016
-
[17]
Y .-H. Ma, D. Xu, H. Dong, and C.-P. Sun, Universal constraint for efficiency and power of a low-dissipation heat engine, Phys. Rev. E 98, 042112 (2018)
work page 2018
-
[18]
H. Yuan, Y .-H. Ma, and C. P. Sun, Optimizing thermody- namic cycles with two finite-sized reservoirs, Phys. Rev. E105, L022101 (2022)
work page 2022
-
[19]
R.-X. Zhai, F.-M. Cui, Y .-H. Ma, C. P. Sun, and H. Dong, Experimental test of power-efficiency trade-off in a finite-time Carnot cycle, Phys. Rev. E 107, L042101 (2023)
work page 2023
-
[20]
Y .-H. Ma and C. Fu, Unified approach to power-efficiency trade-off of generic thermal machines, arXiv preprint arXiv:2411.03849 10.48550/arXiv.2411.03849 (2024)
-
[21]
I. Reyes-Ramírez, M. A. Barranco-Jiménez, A. Rojas-Pacheco, and L. Guzmán-Vargas, Global stability analysis of a curzon– ahlborn heat engine under different regimes of performance, Entropy 16, 5796 (2014)
work page 2014
-
[22]
Bejan, Entropy Generation Minimization (CRC Press, Boca Raton, Fla., 1996)
A. Bejan, Entropy Generation Minimization (CRC Press, Boca Raton, Fla., 1996)
work page 1996
-
[23]
B. Andresen, P. Salamon, and R. S. Berry, Thermodynamics in finite time: Extremals for imperfect heat engines, J. Chem. Phys. 66, 1571 (1977)
work page 1977
-
[24]
R. S. Berry, P. Salamon, and B. Andresen, eds., Finite-Time Thermodynamics (MDPI - Multidisciplinary Digital Publishing Institute, 2022)
work page 2022
discussion (0)
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