A non-endoreversible Otto cycle model: improving power output and efficiency

We propose a finite-time thermodynamics model for an Otto thermal cycle. Our model considers global losses in a simplified way lumped into a friction-like term, and takes into account the departure from an endoreversible regime through a parameter (R) arising from the Clausius inequality. Our numerical results suggest that the cycle's power output and efficiency are very sensitive to that parameter. We find that R is the ratio of the constant-volume heat capacities of the reactants and products in the combustion reaction occurring inside the working fluid. Our results have implications in the search for new fuels for internal combustion engines.

[1]  Jincan Chen THE MAXIMUM POWER OUTPUT AND MAXIMUM EFFICIENCY OF AN IRREVERSIBLE CARNOT HEAT ENGINE , 1994 .

[2]  Karl Heinz Hoffmann,et al.  Optimal paths for thermodynamic systems: The ideal diesel cycle , 1982 .

[3]  Jincan Chen,et al.  Optimal performance of an endoreversible‐combined refrigeration cycle , 1988 .

[4]  F. Angulo-Brown,et al.  Compression ratio of an optimized air standard Otto-cycle model , 1994 .

[5]  H. Yavuz,et al.  Finite-time thermodynamic analysis of a radiative heat engine with internal irreversibility , 1994 .

[6]  Fernando Angulo-Brown,et al.  Endoreversible thermal cycle with a nonlinear heat transfer law , 1993 .

[7]  Stanislaw Sieniutycz,et al.  Finite-time thermodynamics and thermoeconomics , 1990 .

[8]  R S Berry,et al.  Finite-time thermodynamics: Engine performance improved by optimized piston motion. , 1981, Proceedings of the National Academy of Sciences of the United States of America.

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

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

[11]  Santiago Velasco,et al.  On an irreversible air standard Otto-cycle model , 1995 .

[12]  Harvey S. Leff,et al.  Thermal efficiency at maximum work output: New results for old heat engines , 1987 .

[13]  M. Rubin Optimal configuration of a class of irreversible heat engines. II , 1979 .

[14]  Yehuda B. Band,et al.  The generalized Carnot cycle: A working fluid operating in finite time between finite heat sources and sinks , 1983 .