Performance analysis of an irreversible Miller cycle with considerations of relative air–fuel ratio and stroke length

Abstract The performance of an air standard Miller cycle is analyzed using finite-time thermodynamics. The results show that if compression ratio exceeds certain value, the power output first increases and then starts to decrease with increasing relative air–fuel ratio, while if compression ratio exceeds certain value, the power output decreases with increasing relative air–fuel ratio. The results also show that if compression ratio is less than certain value, the power output decreases with increasing stroke length, while if compression ratio exceeds certain value, the power output first increases and then starts to decrease with increasing stroke length. With further increase in compression ratio, the increase of stroke length results in decreasing the power output. The results obtained from this work can be helpful in the design and evaluation of practical Miller engines.

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

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

[3]  Adnan Parlak,et al.  Comparative performance analysis of irreversible Dual and Diesel cycles under maximum power conditions , 2005 .

[4]  G. H. Abd Alla Computer simulation of a four stroke spark ignition engine , 2002 .

[5]  Bahri Sahin,et al.  Performance optimisation of an irreversible dual cycle with respect to pressure ratio and temperature ratio––experimental results of a ceramic coated IDI Diesel engine , 2004 .

[6]  F. Sun,et al.  Unified thermodynamic description and optimization for a class of irreversible reciprocating heat engine cycles , 2008 .

[7]  Chih Wu,et al.  Performance analysis and optimization of a supercharged Miller cycle Otto engine , 2003 .

[8]  Fengrui Sun,et al.  Effects of heat transfer and friction on the performance of an irreversible air-standard miller cycle , 2005 .

[9]  A. Al-Sarkhi,et al.  Efficiency of a Miller engine , 2006 .

[10]  Lingen Chen,et al.  Finite time exergoeconomic performance for six endoreversible heat engine cycles: Unified description , 2011 .

[11]  Bilal Akash,et al.  Performance evaluation of irreversible Miller engine under various specific heat models , 2007 .

[12]  Lingen Chen,et al.  Power, efficiency, entropy-generation rate and ecological optimization for a class of generalized irreversible universal heat-engine cycles , 2007 .

[13]  Lingen Chen,et al.  Finite-time thermodynamic modeling and analysis for an irreversible Dual cycle , 2009, Math. Comput. Model..

[14]  Fengrui Sun,et al.  Optimal paths for minimizing entransy dissipation during heat transfer processes with generalized radiative heat transfer law , 2010 .

[15]  L. Chen,et al.  Effects of heat transfer and variable specific heats of working fluid on performance of a Miller cycle , 2005 .

[16]  Fengrui Sun,et al.  Performance of an Atkinson cycle with heat transfer, friction and variable specific-heats of the working fluid , 2006 .

[17]  Fengrui Sun,et al.  Performance of Diesel cycle with heat transfer, friction and variable specific heats of working fluid , 2007 .

[18]  Lingen Chen,et al.  Reciprocating heat-engine cycles , 2005 .

[19]  Fengrui Sun,et al.  Endoreversible radiative heat engine configuration for maximum efficiency , 2010 .

[20]  J. Liu,et al.  Optimum performance analysis of a class of typical irreversible heat engines with temperature-dependent heat capacities of the working substance , 2010 .

[21]  Adnan Parlak,et al.  The effect of heat transfer on performance of the Diesel cycle and exergy of the exhaust gas stream in a LHR Diesel engine at the optimum injection timing , 2005 .

[22]  Shuhn-Shyurng Hou,et al.  Performance analysis of an air-standard Miller cycle with considerations of heat loss as a percentage of fuel's energy, friction and variable specific heats of working fluid , 2008 .

[23]  Masakazu Sasaki,et al.  Development of capacitor hybrid system for urban buses , 2002 .

[24]  Ugur Kesgin,et al.  Efficiency improvement and NOx emission reduction potentials of two‐stage turbocharged Miller cycle for stationary natural gas engines , 2005 .

[25]  Yingru Zhao,et al.  Performance analysis of an irreversible Miller heat engine and its optimum criteria , 2007 .

[26]  Fengrui Sun,et al.  Finite-time thermodynamic modelling and analysis for an irreversible Miller cycle , 2011 .

[27]  John B. Heywood,et al.  Internal combustion engine fundamentals , 1988 .

[28]  Andrew L. Emtage,et al.  The Calculation of Heat Release Energy from Engine Cylinder Pressure Data , 1998 .

[29]  Tsuyoshi Goto,et al.  A study of the improvement effect of Miller-cycle on mean effective pressure limit for high-pressure supercharged gasoline engines , 1997 .

[30]  Fengrui Sun,et al.  Effects of heat transfer, friction and variable specific heats of working fluid on performance of an irreversible dual cycle , 2006 .

[31]  A. Al-Sarkhi,et al.  EFFICIENCY OF MILLER ENGINE AT MAXIMUM POWER DENSITY , 2002 .

[32]  Kengo Tanaka,et al.  Development of High Efficiency Miller Cycle Gas Engine , 2001 .