1990
DOI: 10.1088/0022-3727/23/2/002
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A class of irreversible Carnot refrigeration cycles with a general heat transfer law

Abstract: The performance of a class of irreversible Carnot refrigeration cycles operating between two heat reservoirs at a low temperature T, and a high temperature TH, for which the oniy irreversibility results from the finite rate of heat conduction, is studied. The relation between the optimal rate of refrigeration and the coefficient of performance of these cycles is derived, based on a general heat transfer law. Moreover, the optimal performance of these cycles is discussed and the effect of different heat transfe… Show more

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Cited by 176 publications
(144 citation statements)
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“…(3.12) and the picture in Fig. 1(b), the entropy change per unit time of the extended system can be expressed in canonical form (11) provided that we use the corresponding relations d [49]. Assume that N electrons flow through the generator during time interval τ .…”
Section: Conclusion and Discussionmentioning
confidence: 99%
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“…(3.12) and the picture in Fig. 1(b), the entropy change per unit time of the extended system can be expressed in canonical form (11) provided that we use the corresponding relations d [49]. Assume that N electrons flow through the generator during time interval τ .…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…The other classic topic on nonequilibrium processes is finite-time thermodynamics [4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21] which is concerned * Corresponding author. Email: tuzc@bnu.edu.cn mainly with the energy conversion efficiency for heat devices including heat engines and refrigerators that complete thermodynamic cycles in finite time or operate in finite net rate.…”
Section: Introductionmentioning
confidence: 99%
“…To transfer heat from the cold bath to the hot bath, work has to be done on the system and hence, we have W = Q h + Q c < 0. The coefficient of performance (COP) is defined as ζ = Q c /|W| [50,51].…”
Section: Performance As a Refrigeratormentioning
confidence: 99%
“…(11), (12), (13), and (14), together with use of Eqs. (15), (16), and (17), we can derive after some simple reshuffling,…”
Section: Optimum Analysismentioning
confidence: 99%
“…Various optimization criteria [16][17][18][19][20][21][22] have been proposed in optimum analysis of a classical or quantum refrigeration cycle. Chen and Yan [16] introduced the function χ = εQ c /τ , with Q c the heat transported from the cold reservoir and τ the cycle time, as a target function within finite-time-thermodynamics context. Velasco et al [17] adopted the per-unit-time COP as a target function while Allahverdyan et al [18] introduced εQ c to be the target function.…”
Section: Introductionmentioning
confidence: 99%