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By J R Bowen; N Manson; American Institute of Aeronautics and Astronautics.; Congrès. Poitiers. 1983

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Extra resources for Dynamics of flames and reactive systems. Technical Papers presented from the Ninth International Colloquium on Gasdynamics of Explosions and Reactive Systems, Poitiers, France, July 1983

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1962) On diffusional thermal instability of laminar flame. Zh. Prikl. Mekh. Tekh. Fiz. 2(4), 21-26. Bowen, J. , and Oppenheim, A. K. (1963) Singular perturbation refinement to quasi-steady-state'approximation in chemical kinetics. Chemical Engineering Science 18, 177-188, Pergamon Press, Oxford, England. Boys, S. F. and Corner, J. (1949) The structure of the reaction zone in a flame. Proc. R. Soc. A 197(1048), 90-106. Buckmaster, J. D. (1976) The quenching of deflagration waves. Combust. Flame'26(2), 151-162.

Seventh International) Symposium on Combustion, Butterworths, London, 339-341. , Clavin, P. and Boyer, L. (1983) The hydrodynamical coupling between the motion of a flame front and the upstream gas flow. Phys. Rev. Lett. 51(16), 1450-1453. , Clavin, P. and Boyer, L. (1983)'The feed-back of a flame front on turbulent flows. Proceedings of the IX International Colloquium on Dynamics of Explosions and Reactive Systems, July 3-8, 1983, Poitiers, France. MODERN LAMINAR FLAMETHEORY 33 Searby, G. and Clavin, P.

1. The one and only d i f f i c u l t y left is the accurate determination of the upper bound of Eq. (I8b) corresponding to the boundary between the reaction zone and the preheated region. This is a matching problem that can be solved systematically by the appropriate techniques of asymptotic expansion (Van Dyke 1975; Cole 1968) that was not known in 1938. In spite of that, with an excellent sense of physics, in 1938 ZFK gave the correct answer for the limiting case of 3=°°. Noting that lim i = / dE H n e~~ = r ( n + 1 ) ( = n !

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