TY - JOUR
T1 - Discussion of a Wrinkled Laminar Flamelet Model in a Diffusion Flame in Grid Turbulence
AU - Manako, Hiroyasu
AU - Ueda, Toshihisa
AU - Mizomoto, Masahiko
PY - 1990
Y1 - 1990
N2 - The temperature has been measured in a field in which laminar hydrogen (6.0 m/s at the center of a burner exit) was injected into a co-flowing air stream (6.0 m/s) with some kinds of grid turbulence. It is shown that the ratio of a laminar flame length to the turbulent one is proportional to the turbulent Reynolds number, Re., (integral scale is considered a characteristic length) in the measured extent (Rel≤ 1 000), and therefore that the integral scale of a reactant flow is an important parameter for the flames in this paper. The width of a flame displacement is estimated from the temperature profiles when the flame is assumed to be a wrinkled laminar flamelet. The width is also measured directly by a flow visualization method. Both the widths obtained by the two different methods agree well with each other. This fact indicates that the turbulent flame in this paper can be treated as a wrinkled laminar flamelet.
AB - The temperature has been measured in a field in which laminar hydrogen (6.0 m/s at the center of a burner exit) was injected into a co-flowing air stream (6.0 m/s) with some kinds of grid turbulence. It is shown that the ratio of a laminar flame length to the turbulent one is proportional to the turbulent Reynolds number, Re., (integral scale is considered a characteristic length) in the measured extent (Rel≤ 1 000), and therefore that the integral scale of a reactant flow is an important parameter for the flames in this paper. The width of a flame displacement is estimated from the temperature profiles when the flame is assumed to be a wrinkled laminar flamelet. The width is also measured directly by a flow visualization method. Both the widths obtained by the two different methods agree well with each other. This fact indicates that the turbulent flame in this paper can be treated as a wrinkled laminar flamelet.
KW - Diffusion Combustion
KW - Flame
KW - Integral Scale
KW - Wrinkled Laminar Flamelet Grid Turbulence
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U2 - 10.1299/kikaib.56.3080
DO - 10.1299/kikaib.56.3080
M3 - Article
AN - SCOPUS:85024347986
SN - 0387-5016
VL - 56
SP - 3080
EP - 3086
JO - Nihon Kikai Gakkai Ronbunshu, B Hen/Transactions of the Japan Society of Mechanical Engineers, Part B
JF - Nihon Kikai Gakkai Ronbunshu, B Hen/Transactions of the Japan Society of Mechanical Engineers, Part B
IS - 530
ER -