Unified cycle model of a class of internal combustion engines and their optimum performance characteristics

Shiyan ZHENG

PDF(277 KB)
PDF(277 KB)
Front. Energy ›› 2011, Vol. 5 ›› Issue (4) : 367-375. DOI: 10.1007/s11708-011-0170-x
RESEARCH ARTICLE
RESEARCH ARTICLE

Unified cycle model of a class of internal combustion engines and their optimum performance characteristics

Author information +
History +

Abstract

The unified cycle model of a class of internal combustion engines is presented, in which the influence of the multi-irreversibilities mainly resulting from the adiabatic processes, finite-time processes and heat leak loss through the cylinder wall on the performance of the cycle are taken into account. Based on the thermodynamic analysis method, the mathematical expressions of the power output and efficiency of the cycle are calculated and some important characteristic curves are given. The influence of the various design parameters such as the high-low pressure ratio, the high-low temperature ratio, the compression and expansion isentropic efficiencies etc. on the performance of the cycle is analyzed. The optimum criteria of some important parameters such as the power output, efficiency and pressure ratio are derived. The results obtained from this unified cycle model are very general and useful, from which the optimal performance of the Atkinson, Otto, Diesel, Dual and Miller heat engines and some new heat engines can be directly derived.

Keywords

internal combustion engine / irreversibility / power output / efficiency / optimization

Cite this article

Download citation ▾
Shiyan ZHENG. Unified cycle model of a class of internal combustion engines and their optimum performance characteristics. Front Energ, 2011, 5(4): 367‒375 https://doi.org/10.1007/s11708-011-0170-x

References

[1]
Wu C, Chen L, Chen J. Recent Advances in Finite-Time Thermodynamics. New York: Nova Science Publishers, Inc., 1999
[2]
Bejan A. Advanced Engineering Thermodynamics. 2nd ed. New York: Wiley, 1996
[3]
Moran M J, Shapiro H N. Fundamentals of Engineering Thermodynamics. 2nd ed. New York: Wiley, 1992
[4]
Mozurkewich M, Stephen B. Optimal paths for thermodynamic systems: The ideal Otto cycle. Journal of Applied Physics, 1982, 53(1): 34-42
CrossRef Google scholar
[5]
Angulo-Brown F, Rocha-Martínez J, Navarrete-González T D, Navarrete- González T. A non-endoreversible Otto cycle model: improving power output and efficiency. Journal of Physics D, Applied Physics, 1996, 29(1): 80-83
CrossRef Google scholar
[6]
Chen L, Wu C, Sun F R, Cao S. Heat transfer effects on the net work output and efficiency characteristics for an air-standard Otto cycle. Energy Conversion and Management, 1998, 39(7): 643-648
CrossRef Google scholar
[7]
Bhattacharyya S. Optimizing an irreversible Diesel cycle—fine tuning of compression ratio and cut-off ratio. Energy Conversion and Management, 2000, 41(8): 847-854
CrossRef Google scholar
[8]
Akash B. Effect of heat transfer on the performance of an air-standard Diesel cycle. International Communications in Heat and Mass Transfer, 2001, 28(1): 87-95
CrossRef Google scholar
[9]
Ge Y L, Chen L G, Sun F R, Wu C. Reciprocating heat-engine cycles. Applied Energy, 2005, 81(4): 397-408
CrossRef Google scholar
[10]
Chen J C, Zhao Y R, He J Z. Optimization criteria for the important parameters of an irreversible Otto heat-engine. Applied Energy, 2006, 83(3): 228-238
CrossRef Google scholar
[11]
Zhao Y R, Lin B H, Zhang Y, Chen J C.Performance analysis and parametric optimum design of an irreversible Diesel heat engine. Energy Conversion and Management, 2006, 47(18,19): 3383-3392
[12]
Zhao Y R, Chen J C. Performance analysis and parametric optimum criteria of an irreversible Atkinson heat-engine. Applied Energy, 2006, 83(8): 789-800
CrossRef Google scholar
[13]
Zhao Y R, Chen J C. An irreversible heat engine model including three typical thermodynamic cycles and their optimum performance analysis. International Journal of Thermal Sciences, 2007, 46(6): 605-613
CrossRef Google scholar
[14]
Zhao Y R, Chen J C. Performance analysis of an irreversible Miller heat engine and its optimum criteria. Applied Thermal Engineering, 2007, 27(11,12): 2051-2058
[15]
Chen L G, Wu C, Sun F R.Cooling load versus cop characteristics for an irreversible air refrigeration cycle. Energy Conversion and Management, 1998, 39(1,2): 117-125
[16]
Aragón-González G, Canales-Palma A, León-Galicia A. Maximum irreversible work and efficiency in power cycles. Journal of Physics. D, Applied Physics, 2000, 33(11): 1403-1409
CrossRef Google scholar
[17]
Curzon F, Ahlborn B. Efficiency of a Carnot engine at maximum power output. American Journal of Physics, 1975, 43(1): 22-24
CrossRef Google scholar
[18]
Salamon P, Nitzan A. Finite time optimizations of a Newton’s law Carnot cycle. Journal of Chemical Physics, 1981, 74(6): 3546-3560
CrossRef Google scholar
[19]
Chen J C, Yan Z J. Unified description of endoreversible cycles. Physical Review A: General Physics, 1989, 39(8): 4140-4147
CrossRef Pubmed Google scholar
[20]
Angulo-Brown F, Fernández-Betanzos J, Díaz-Pico C A. Compression ratio of an optimized air standard Otto-cycle model. European Journal of Physics, 1994, 15(1): 38-42
CrossRef Google scholar
[21]
Chen L G, Ge Y L, Sun F R. Unified thermodynamic description and optimization for a class of irreversible reciprocating heat engine cycles. Proceedings of the Institution of Mechanical Engineers. Part D, Journal of Automobile Engineering, 2008, 222(8): 1489-1500
CrossRef Google scholar
[22]
Ebrahimi R. Performance optimization of a Diesel cycle with specific heat ratio. Journal of American Science, 2010, 6(1): 157-161

Acknowledgements

This work was supported by the Key Project of Fujian Service Hercynian Construction (A100) and the Key Subject Construction Funds of Quanzhou Normal University, China.

RIGHTS & PERMISSIONS

2014 Higher Education Press and Springer-Verlag Berlin Heidelberg
AI Summary AI Mindmap
PDF(277 KB)

Accesses

Citations

Detail

Sections
Recommended

/