By J R Bowen; N Manson; American Institute of Aeronautics and Astronautics.; Congrès. Poitiers. 1983
Read or Download 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 PDF
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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
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 !