| 21. | Interestingly, as temperature decreases, the maximum theoretical fuel cell efficiency increases, in contrast to the Carnot cycle.
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| 22. | Entropy is the above-mentioned unexpected and, to some, obscure integral that arises directly from the Carnot cycle.
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| 23. | Hence, no real heat engine could realise the Carnot cycle's reversibility and was condemned to be less efficient.
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| 24. | A reversible thermodynamic cycle for AMTEC shows that it is, at best, slightly less efficient than a Carnot cycle.
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| 25. | A Carnot cycle taking place between a hot reservoir at temperature T H and a cold reservoir at temperature T C.
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| 26. | Practical fossil fuel stations operating as heat engines cannot exceed the Carnot cycle limit for conversion of heat energy into useful work.
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| 27. | Any real heat engine could not realize the Carnot cycle's reversibility, and was condemned to be even less efficient.
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| 28. | A Carnot cycle is a special kind of cyclic process affecting a body composed of material suitable for use in a heat engine.
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| 29. | Theoretical thermal efficiency equals that of the hypothetical Carnot cycle i . e . the highest efficiency attainable by any heat engine.
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| 30. | The remaining residual heat is still high enough to use it in traditional thermalized way via Carnot Cycle e . g . steam turbine.
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