1992
DOI: 10.1063/1.351755
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General performance characteristics of real heat engines

Abstract: Realistic upper bounds can be placed on the power and efficiency of real heat engines via a relatively simple analytic treatment of primary sources of irreversibility. Generalized curves for heat engine performance, their universal nature, and quantitative evaluation of upper bounds for power and efficiency are derived for several engine types, specifically: Brayton cycle (gas turbines), Rankine cycle (steam turbines), and cycles with sizable heat leaks, such as thermoelectric generators. The key irreversibili… Show more

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Cited by 153 publications
(130 citation statements)
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“…The next step of refinement for thermodynamic description of the Earth as a heat engine would be to include a parallel leaky wire (conduction) to the Curzon-Ahlborn engine as for the cases in figures 1, 2 and 4. This case has the interesting property that the maximum efficiency does not coincide with the maximum entropy production (Gordon & Huleihil 1992).…”
Section: Discussionmentioning
confidence: 99%
“…The next step of refinement for thermodynamic description of the Earth as a heat engine would be to include a parallel leaky wire (conduction) to the Curzon-Ahlborn engine as for the cases in figures 1, 2 and 4. This case has the interesting property that the maximum efficiency does not coincide with the maximum entropy production (Gordon & Huleihil 1992).…”
Section: Discussionmentioning
confidence: 99%
“…Heat leakage is of primary importance for the performance of heat engines as has been shown by Andresen et al [17] and pursued by Patria et al [18]; Chen et al also used models with heat losses to develop the general performance characteristics of engines as was first shown by Gordon and Huleikil [19]. Two characteristic points show up clearly on the curve representing power output versus first law efficiency.…”
Section: Finite Time Thermodynamics (Ftt)mentioning
confidence: 99%
“…Similar to the characteristics of the real conventional irreversible heat engines [39][40][41][42][43], the curves of P * versus η are all closed loop-shaped ones and there exist two important points of states: the maximum power point (η P * ,P * max ) and the maximum efficiency point (η max ,P * η ). When the Brownian heat engine is operating in the regions U ≤ U η and U ≥ U P * , the power output will increase with the increase of efficiency.…”
Section: Power Versus Efficiency Characteristic Without External Forcementioning
confidence: 99%