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大褶皱极限下波纹火焰的西瓦申斯基方程。

Sivashinsky equation for corrugated flames in the large-wrinkle limit.

作者信息

Joulin Guy, Denet Bruno

机构信息

Laboratoire de Combustion et de Détonique, UPR 9028 du CNRS, ENSMA, 1 rue Clément Ader, B.P. 40109, 86961 Futuroscope Cedex, Poitiers, France.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2008 Jul;78(1 Pt 2):016315. doi: 10.1103/PhysRevE.78.016315. Epub 2008 Jul 23.

DOI:10.1103/PhysRevE.78.016315
PMID:18764058
Abstract

Sivashinsky's [Acta Astron. 4, 1177 (1977)] nonlinear integrodifferential equation for the shape of corrugated one-dimensional flames is ultimately reducible to a 2N -body problem, involving the 2N complex poles of the flame slope. Thual, Frisch, and Hénon [J. Phys. (France) 46, 1485 (1985)] derived singular linear integral equations for the pole density in the limit of large steady wrinkles (N>>1) , which they solved exactly for monocoalesced periodic fronts of highest amplitude of wrinkling and approximately otherwise. Here we solve those analytically for isolated crests, next for monocoalesced, then bicoalesced periodic flame patterns, whatever the (large) amplitudes involved. We compare the analytically predicted pole densities and flame shapes to numerical results deduced from the pole-decomposition approach. Good agreement is obtained, even for moderately large Ns . The results are extended to give hints as to the dynamics of supplementary poles. Open problems are evoked.

摘要

西瓦申斯基[《天文学学报》4, 1177 (1977)]关于波纹状一维火焰形状的非线性积分微分方程最终可简化为一个2N体问题,该问题涉及火焰斜率的2N个复极点。图阿尔、弗里施和埃农[《法国物理杂志》46, 1485 (1985)]推导了在大稳态皱纹极限(N>>1)下极点密度的奇异线性积分方程,他们精确求解了皱纹幅度最大的单合并周期前沿,其他情况则近似求解。在此,我们针对孤立波峰解析求解这些方程,接着求解单合并、然后是双合并周期火焰模式,无论涉及的(大)幅度如何。我们将解析预测的极点密度和火焰形状与从极点分解方法推导的数值结果进行比较。即使对于适度大的N值,也能得到良好的一致性。结果得到扩展,以给出关于补充极点动力学的提示。引出了一些未解决的问题。

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