Power and efficiency analysis of an endoreversible closed intercooled regenerated Brayton cycle

In this paper, finite-time thermodynamics (FTT) is applied to analyse the performance of an endoreversible closed intercooled regenerated Brayton cycle coupled with variable-temperature heat reservoirs. The analytical formulae of dimensionless power and efficiency are thus derived. The intercooling pressure ratio is optimised for maximum power and maximum efficiency, respectively. The effects of component (the intercooler, the regenerator and the hot- and cold-side heat exchangers) effectiveness; the thermal capacity rate of the working fluid; the heat reservoir inlet temperature ratio; the inlet temperature ratio of the cooling fluid in the intercooler and the cold-side heat reservoir on maximum power and its corresponding efficiency and corresponding intercooling pressure ratio, as well as maximum efficiency and its corresponding power and corresponding intercooling pressure ratio are analysed by detailed numerical examples. Some results in the recent FTT literature are replicated.

[1]  Cha'o-Kuang Chen,et al.  Maximum power of an endoreversible intercooled Brayton cycle , 2000 .

[2]  A. Bejan Theory of heat transfer-irreversible power plants , 1988 .

[3]  Lingen Chen,et al.  Effect of heat resistance on the performance of closed gas turbine regenerative cycles , 1999 .

[4]  Sergio Sibilio,et al.  Recent Advances in Finite-Time Thermodynamics , 1999 .

[5]  Fengrui Sun,et al.  Power density analysis and optimization of a regenerated closed variable-temperature heat reservoir Brayton cycle , 2001 .

[6]  I. I. Novikov The efficiency of atomic power stations (a review) , 1958 .

[7]  Fengrui Sun,et al.  Performance comparison of an irreversible closed Brayton cycle under maximum power density and maximum power conditions , 2002 .

[8]  A. Bejan Advanced Engineering Thermodynamics , 1988 .

[9]  A. D. Vos,et al.  Endoreversible thermodynamics of solar energy conversion , 1992 .

[10]  Fengrui Sun,et al.  Power Density Optimization for an Irreversible Regenerated Closed Brayton Cycle , 2001 .

[11]  A. Bejan Entropy generation minimization: The new thermodynamics of finite-size devices and finite-time processes , 1996 .

[12]  Santiago Velasco,et al.  Optimum performance of a regenerative Brayton thermal cycle , 1997 .

[13]  Lingen Chen,et al.  Finite Time Thermodynamic Optimization or Entropy Generation Minimization of Energy Systems , 1999 .

[14]  Chen Lin-gen Finite Time Thermodynamic Analyses for Gas Turbine Cycle:Theory and Application , 2001 .

[15]  F. Curzon,et al.  Efficiency of a Carnot engine at maximum power output , 1975 .

[16]  P. Chambadal Les centrales nucléaires , 1957 .

[17]  Stanislaw Sieniutycz,et al.  Thermodynamics of energy conversion and transport , 2000 .

[18]  Fengrui Sun,et al.  Effect of heat transfer law on the performance of a generalized irreversible Carnot engine , 1999 .

[19]  S. Sieniutycz,et al.  Thermodynamic Optimization of Finite-Time Processes , 2000 .

[20]  Cha'o-Kuang Chen,et al.  Power Optimization of an Irreversible Brayton Heat Engine , 1997 .