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Influence of hydrodynamics and diffusion upon the stability limits of laminar premixed flames

Published online by Cambridge University Press:  20 April 2006

Pierre Pelce
Affiliation:
Laboratoire de Dynamique et Thermophysique des Fluides (LA 72). Université de Provence, Centre St Jérôme, rue H. Poincaré, 13397 Marseille cedex 13, France
Paul Clavin
Affiliation:
Laboratoire de Dynamique et Thermophysique des Fluides (LA 72). Université de Provence, Centre St Jérôme, rue H. Poincaré, 13397 Marseille cedex 13, France

Abstract

An analytical theory is developed for the stability properties of planar fronts of premixed laminar flames freely propagating downwards in a uniform reacting mixture. The coupling between the hydrodynamics and the diffusion process is described for an arbitrary expansion of the gas across the flame. Viscous effects are included with an arbitrary Prandtl number. The flame structure is described for a large value of the reduced activation energy and for a Lewis number close to unity. The flame thickness is assumed to be small compared with the wavelength of the wrinkles of the front, this wavelength being also the characteristic lengthscale of the perturbations of the flow field outside the flame. A two-scale method is then used to solve the problem. The results show that the acceleration of gravity associated with the diffusion mechanisms inside the front can counterbalance the hydrodynamical instability when the laminar-flame velocity is low enough. The theory provides predictions concerning the instability threshold. In particular, the dimensions of the cells are predicted to be large compared with the flame thickness, and thus the basic assumption of the theory is verified. Furthermore, the quantitative predictions are in good agreement with the existing experimental data.

The bifurcation is shown to be of a different nature than predicted by the purely diffusive–thermal model.

The viscous diffusivities are supposed to be independent of the temperature, and then the viscosity is proved to have no effect at all on the dynamical properties of the flame front.

Type
Research Article
Copyright
© 1982 Cambridge University Press

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