2000
DOI: 10.1021/ed077p1027
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A Simple Approach to Heat Engine Efficiency

Abstract: Temperature-entropy (TS) diagrams are introduced as a way to simplify the calculation of efficiency for reversible heat engines. The equation for the efficiency of the Stirling cycle is derived from its TS diagram. The conflict over the efficiency of the Stirling cycle is thereby resolved; the standard Stirling cycle does not have an efficiency equal to the Carnot cycle efficiency. The historical confusion about the efficiency of the Stirling cycle is shown to arise from two sources: a careless definition of h… Show more

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Cited by 4 publications
(3 citation statements)
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“…Returning to figure 1, only the heat transfers denoted Q H and Q C are with the external temperature reservoirs (connected to the ambient surroundings at temperature T H and to the cooling load at T C ). The regenerator has obviated the need for other reservoirs at intermediate temperatures between T H and T C during the isochoric processes [12]. Therefore, calculating the COP as the ratio of the 'energy transfer wanted' to the 'energy transfer paid for' gives…”
mentioning
confidence: 99%
“…Returning to figure 1, only the heat transfers denoted Q H and Q C are with the external temperature reservoirs (connected to the ambient surroundings at temperature T H and to the cooling load at T C ). The regenerator has obviated the need for other reservoirs at intermediate temperatures between T H and T C during the isochoric processes [12]. Therefore, calculating the COP as the ratio of the 'energy transfer wanted' to the 'energy transfer paid for' gives…”
mentioning
confidence: 99%
“…To show the importance of the clarification made by this proof, one example of a relevant interpretation which may lead to misunderstanding or errors is reviewed here. The example is a comparison between the thermal efficiency of Carnot and Stirling engines using the T-S diagram studied in [5]. In the 'Graphical Efficiency' section of this investigation, Salter presents a proof of the statement on the first page of the paper as 'Stirling cycles and other reversible cycles cannot have an efficiency equaling the Carnot efficiency'.…”
Section: Lemma 2 For a Cycle Which Operates Totally Reversibly Betwee...mentioning
confidence: 99%
“…Let b represent the variables in question. Then the variance in some function f(b) is given by [10][11][12][13][14] s f 2 = g T V g, (2) in which the elements of g are g i = ∂f/∂b i , and V is the variance-covariance matrix of the variables b. For example, in the calculation of the error in the linear calibration fit function itself (f = a + bx), g 1 = 1 and g 2 = x if b 1 is taken to be a and b 2 is b.…”
Section: Error Propagation In Functions Of Correlated Variablesmentioning
confidence: 99%