TY - JOUR
T1 - On the Wind Generated by a Collapsing Diffusion Flame
AU - Buckmaster, J.
AU - Stewart, D. S.
AU - Ignatiadis, A.
AU - Williams, M.
N1 - Funding Information:
This work was supported by the National Science Foundation. and by the Army Research Office. J.B. was supported by a Humboldt Foundation U.S. Senior.Scientist Award while this work was being completed.
PY - 1986/4/20
Y1 - 1986/4/20
N2 - We examine the stationary spherical diffusion flame attached to a fuel drop, and consider the consequences of an instantaneous reduction of the Damkohler number below the extinction threshold, so that steady vigorous burning is no longer possible. Extinction occurs in two stages that are described by a combination of analysis and numerical calculation, valid in the limit of infinite activation energy. The first stage is characterized by a small but very rapid drop in the flame temperature, and a corresponding small but rapid density increase within the reaction zone or flame sheet. The associated increase in mass within the sheet is fed by an unsteady 0(1) velocity field, induced beyond the sheet, and superimposed on the initial 0(1) velocity defined by the steady state. This induced velocity is responsible, in due course, for the drawing in of fluid from infinity towards the collapsing flame. The second stage takes over once reaction becomes negligible, and is characterized by the dispersion of the temperature field through diffusion and advection. This is a rather slow process.
AB - We examine the stationary spherical diffusion flame attached to a fuel drop, and consider the consequences of an instantaneous reduction of the Damkohler number below the extinction threshold, so that steady vigorous burning is no longer possible. Extinction occurs in two stages that are described by a combination of analysis and numerical calculation, valid in the limit of infinite activation energy. The first stage is characterized by a small but very rapid drop in the flame temperature, and a corresponding small but rapid density increase within the reaction zone or flame sheet. The associated increase in mass within the sheet is fed by an unsteady 0(1) velocity field, induced beyond the sheet, and superimposed on the initial 0(1) velocity defined by the steady state. This induced velocity is responsible, in due course, for the drawing in of fluid from infinity towards the collapsing flame. The second stage takes over once reaction becomes negligible, and is characterized by the dispersion of the temperature field through diffusion and advection. This is a rather slow process.
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U2 - 10.1080/00102208608959798
DO - 10.1080/00102208608959798
M3 - Article
AN - SCOPUS:84889217493
SN - 0010-2202
VL - 46
SP - 145
EP - 165
JO - Combustion Science and Technology
JF - Combustion Science and Technology
IS - 3-6
ER -