1987
DOI: 10.1080/00102208708947045
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Instabilities in Upward Propagating Flames

Abstract: A derivation is presented of a nonlinear evolution equation describing the dynamics of a flame front propagating in a vertical channel:where G is the buoyancy parameter and iii the average of eJ> over the channel cross-section. The velocity and equilibrium form of the distorted flame front are calculated, and the effect of the suppression of cellular structure in upward propagating flames is described.

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Cited by 42 publications
(16 citation statements)
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“…The Rayleigh-Taylor instability, caused by a heavier fluid placed on top of a lighter one, appears in a wide variety of physical systems, such as laser ablation [1,2], astrophysics [3], liquid-gas interfaces [4], combustion [5,6], and chemical reaction fronts [7,8]. The fluids involved are usually separated by an interface that contains a stabilizing mechanism, such as surface tension [9] or molecular diffusivity (as in the case of a chemical front) [10].…”
Section: Introductionmentioning
confidence: 99%
“…The Rayleigh-Taylor instability, caused by a heavier fluid placed on top of a lighter one, appears in a wide variety of physical systems, such as laser ablation [1,2], astrophysics [3], liquid-gas interfaces [4], combustion [5,6], and chemical reaction fronts [7,8]. The fluids involved are usually separated by an interface that contains a stabilizing mechanism, such as surface tension [9] or molecular diffusivity (as in the case of a chemical front) [10].…”
Section: Introductionmentioning
confidence: 99%
“…As a mathematical model we shall employ the weakly nonlinear flame interface evolution equation similar to that proposed by Rakib and Sivashinsky [18]. In Appendix B, we specify the framework of approximation and carry out the formal derivation of the equation-which appears here for the first time.…”
Section: Introductionmentioning
confidence: 99%
“…has gotten a lot of attention and interest from both the engineering and the mathematical communities to model several problems including but not limited to the control of turbulent flow [2,9], the excitation of long water waves by a moving pressure distribution [1], the dispersal of a population [32], and the behavior of the flame front interface under physical assumption [29]. Rakib and Sivashinsky [29] derived a nonlinear evolution equation as a model for the flame front interface:…”
Section: Introductionmentioning
confidence: 99%