The Effects of Cycle Temperature and Cycle Pressure Ratios on the Performance of an Irreversible Otto Cycle

This paper reports the thermodynamic optimization based on the maximum mean effective pressure, maximum power and maximum thermal efficiency criteria for an irreversible Otto heat engine model which includes internal irreversibility resulting from the adiabatic processes. The mean effective pressure, power output, and thermal efficiency are obtained by introducing the compression ratio, cycle temperature ratio, specific heat ratio and the compression and expansion efficiencies. Optimal performance and design parameters of the Otto cycle are obtained analytically for the maximum power and maximum thermal efficiency conditions and numerically for the maximum mean effective pressure conditions. The results at maximum mean effective pressure conditions are compared with those results obtained by using the maximum power and maximum thermal efficiency criteria. The effects of the cycle temperature ratio and cycle pressure ratio on the general and optimal performances are investigated.

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

[2]  Lingen Chen,et al.  Heat transfer effects on the net work output and efficiency characteristics for an air-standard Otto cycle , 1998 .

[3]  Fernando Angulo-Brown,et al.  A non-endoreversible Otto cycle model: improving power output and efficiency , 1996 .

[4]  Bjarne Andresen,et al.  Thermodynamics in finite time , 1984 .

[5]  Bahri Sahin,et al.  Optimization of thermal systems based on finite-time thermodynamics and thermoeconomics , 2004 .

[6]  Fengrui Sun,et al.  The effects of variable specific heats of working fluid on the performance of an irreversible Otto cycle , 2005 .

[7]  Yingru Zhao,et al.  Optimization criteria for the important parameters of an irreversible Otto heat-engine , 2006 .

[8]  Osman Azmi Ozsoysal,et al.  Heat loss as a percentage of fuel’s energy in air standard Otto and Diesel cycles , 2006 .

[9]  Sanford Klein,et al.  An Explanation for Observed Compression Ratios in Internal Combustion Engines , 1991 .

[10]  Andrew G. Glen,et al.  APPL , 2001 .

[11]  Chih Wu,et al.  Optimization of the endoreversible otto cycle with respect to both power and mean effective pressure , 1993 .

[12]  Shuhn-Shyurng Hou,et al.  Effects of heat loss as percentage of fuel’s energy, friction and variable specific heats of working fluid on performance of air standard Otto cycle , 2008 .

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

[14]  Fengrui Sun,et al.  Finite-time thermodynamic modelling and analysis of an irreversible Otto-cycle , 2008 .

[15]  Lingen Chen,et al.  Thermodynamic simulation of performance of an Otto cycle with heat transfer and variable specific heats of working fluid , 2005 .

[16]  Shuhn-Shyurng Hou,et al.  Comparison of performances of air standard Atkinson and Otto cycles with heat transfer considerations , 2007 .

[17]  Metin Gumus,et al.  Efficiency of an Otto engine under alternative power optimizations , 2009 .

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