TY - JOUR
T1 - The propagation of a laminar reaction front during end-gas auto-ignition
AU - Martz, Jason B.
AU - Lavoie, George A.
AU - Im, Hong G.
AU - Middleton, Robert J.
AU - Babajimopoulos, Aristotelis
AU - Assanis, Dionissios N.
N1 - Funding Information:
This work was sponsored by the Department of Energy under the University Consortium on Low Temperature Combustion for High Efficiency, Ultra-Low Emission Engines, directed by the University of Michigan under agreement DE-FC26-06NT42629. The authors gratefully acknowledge Professor J.Y. Chen of University of California, Berkeley for providing the skeletal isooctane mechanism, and Drs. William Pitz and Charles Westbrook of The Lawrence Livermore National Laboratory for the provision of HCT and discussions on the topic. The authors also wish to thank Dr. David Reuss of the University of Michigan for the many helpful discussions.
PY - 2012/6
Y1 - 2012/6
N2 - A transient, one dimensional premixed laminar reaction front is used as a model problem to further understand the physical processes influencing reaction front propagation during the various stages of spark-assisted compression ignition (SACI) combustion for both constant and variable domain pressures. This approach is consistent with the wrinkled laminar flame representation of turbulent, spark ignited engine combustion. With the proper choice of timescales and pressure rise rate, it applies to the interaction of the flame with auto-igniting end-gas in a typical automotive engine. Under the conditions simulated by a transient flame code, the reaction front begins as a deflagration, propagating into an end-gas with an initially negligible level of reaction progress. The diffusive-reactive nature of the front is maintained until significant levels of end-gas reaction progress, where the burning velocity depends upon the degree of pre-reaction. At the time of the end-gas maximum chemical power, the maximum temperature gradient and peak rate of heat conduction within the front diminish to the point where combustion becomes chemically controlled. Although significant increases in burning velocity are observed at the onset of chemically controlled combustion within the front, the end-gas is within one front time from the completion of combustion. As a result, no more than one front thickness is consumed by the apparent propagation of the spontaneous ignition front.
AB - A transient, one dimensional premixed laminar reaction front is used as a model problem to further understand the physical processes influencing reaction front propagation during the various stages of spark-assisted compression ignition (SACI) combustion for both constant and variable domain pressures. This approach is consistent with the wrinkled laminar flame representation of turbulent, spark ignited engine combustion. With the proper choice of timescales and pressure rise rate, it applies to the interaction of the flame with auto-igniting end-gas in a typical automotive engine. Under the conditions simulated by a transient flame code, the reaction front begins as a deflagration, propagating into an end-gas with an initially negligible level of reaction progress. The diffusive-reactive nature of the front is maintained until significant levels of end-gas reaction progress, where the burning velocity depends upon the degree of pre-reaction. At the time of the end-gas maximum chemical power, the maximum temperature gradient and peak rate of heat conduction within the front diminish to the point where combustion becomes chemically controlled. Although significant increases in burning velocity are observed at the onset of chemically controlled combustion within the front, the end-gas is within one front time from the completion of combustion. As a result, no more than one front thickness is consumed by the apparent propagation of the spontaneous ignition front.
KW - Auto-ignition
KW - Knock
KW - Laminar burning velocity
KW - Low temperature combustion
KW - Spark assisted compression ignition
KW - Spark ignition
UR - http://www.scopus.com/inward/record.url?scp=84859880268&partnerID=8YFLogxK
U2 - 10.1016/j.combustflame.2012.01.011
DO - 10.1016/j.combustflame.2012.01.011
M3 - Article
AN - SCOPUS:84859880268
SN - 0010-2180
VL - 159
SP - 2077
EP - 2086
JO - Combustion and Flame
JF - Combustion and Flame
IS - 6
ER -