1984
DOI: 10.1016/0017-9310(84)90219-9
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Extinction of premixed flames by stretch and radiative loss

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Cited by 42 publications
(18 citation statements)
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“…(14) and (15) reduce to the previous results of adiabatic tubular flames [20] in the limit of N ¼ 1, R I ¼ 0, and L AE ¼ 0; and those of counterflow flames [3,10] in the limit of N ¼ 0, R I ¼ 0, and R O ! 1.…”
Section: Asymptotic Solutionsupporting
confidence: 50%
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“…(14) and (15) reduce to the previous results of adiabatic tubular flames [20] in the limit of N ¼ 1, R I ¼ 0, and L AE ¼ 0; and those of counterflow flames [3,10] in the limit of N ¼ 0, R I ¼ 0, and R O ! 1.…”
Section: Asymptotic Solutionsupporting
confidence: 50%
“…For both flame geometries, the potential flow assumption, which is commonly used in the large activation energy asymptotic analysis [3,10,20], is employed here. By introducing a geometry factor N with N ¼ 0 for the counterflow flame and N ¼ 1 for the tubular flame (with e R I and e R O being the inner and outer tube radius, respectively), the potential flow field for both configurations can be written as…”
Section: Mathematical Modelmentioning
confidence: 99%
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“…It is therefore of importance to examine the effects of radiative heat loss on stretched flames. Sohrab and Law (1984) investigated the effect of radiative heat loss on stretched premixed flames, and concluded that radiation has little impact on the extinction of stretched flames because the stretch rate in their study was not extended to a sufficiently low value. Egolfopoulos (1994) also studied the radiation effect on steady and unsteady stretched flames, and indicated that radiation is important for near limit stretched laminar flames and for weakly stretched diffusion flames.…”
Section: Introductionmentioning
confidence: 99%