TY - JOUR
T1 - Large eddy simulation of auto-ignition kernel development of transient methane jet in hot co-flow
AU - Liu, Bing
AU - An, Jian
AU - Qin, Fei
AU - Li, Rui
AU - He, Guo Qiang
AU - Shi, Lei
AU - Zhang, Duo
N1 - Publisher Copyright:
© 2020
PY - 2020/5
Y1 - 2020/5
N2 - The auto-ignition process of a transient methane jet issuing into hot co-flow is studied by Large Eddy Simulation (LES). The LES predictions show reasonable agreement with experimental results. A temporal analysis of the transient auto-ignition process is performed, which indicates that the transient auto-ignition process can be divided into four stages in terms of time sequence. The auto-ignition kernel of different times is also analyzed by using Auto-ignition Index, Premixedness Index, and Damköhler number. It reveals that the high temperature region and high release rate region are always located in the flame propagation region and the iso-line of most reactive mixture fraction moves towards the auto-ignition region with the development of auto-ignition kernel. The premixed combustion mainly occurs in the flame propagation region, while premixed combustion and diffusion combustion coexist in the auto-ignition region. At the beginning of the auto-ignition, the Da number of the auto-ignition region is larger than those of the flame propagation region. With the development of the auto-ignition, the Da number of the flame propagation region increases, and larger than the Da number of the auto-ignition region.
AB - The auto-ignition process of a transient methane jet issuing into hot co-flow is studied by Large Eddy Simulation (LES). The LES predictions show reasonable agreement with experimental results. A temporal analysis of the transient auto-ignition process is performed, which indicates that the transient auto-ignition process can be divided into four stages in terms of time sequence. The auto-ignition kernel of different times is also analyzed by using Auto-ignition Index, Premixedness Index, and Damköhler number. It reveals that the high temperature region and high release rate region are always located in the flame propagation region and the iso-line of most reactive mixture fraction moves towards the auto-ignition region with the development of auto-ignition kernel. The premixed combustion mainly occurs in the flame propagation region, while premixed combustion and diffusion combustion coexist in the auto-ignition region. At the beginning of the auto-ignition, the Da number of the auto-ignition region is larger than those of the flame propagation region. With the development of the auto-ignition, the Da number of the flame propagation region increases, and larger than the Da number of the auto-ignition region.
KW - Auto-ignition kernel
KW - Large eddy simulation
KW - Transient auto-ignition
UR - http://www.scopus.com/inward/record.url?scp=85080092501&partnerID=8YFLogxK
U2 - 10.1016/j.combustflame.2020.02.008
DO - 10.1016/j.combustflame.2020.02.008
M3 - 文章
AN - SCOPUS:85080092501
SN - 0010-2180
VL - 215
SP - 342
EP - 351
JO - Combustion and Flame
JF - Combustion and Flame
ER -