arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2006.12947math.NAcs.NA
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格子Boltzmann格式的意外收敛性

Unexpected convergence of lattice Boltzmann schemes

Bruce Boghosian, François Dubois, Benjamin Graille, Pierre Lallemand, Mohamed-Mahdi Tekitek

摘要:

本文数值研究了具有多重弛豫时间的标量D2 Q9格子Boltzmann格式在时间步长与空间步长成正比且趋于零时的收敛性。我们这样做的理论和数值实验相结合。当所有的松弛因子都固定且时间步长趋于零时,经典的形式分析表明,在扩散系数、空间步长和动量弛豫系数之间存在约束的情况下,数值解收敛于热方程的解。如果扩散系数固定,空间步长趋于零,则动量的松弛因子很小,导致前面的分析与数值结果之间的差异。我们提出了一种新的分析方法,这种特定情况下的倏逝波弛豫,基于色散方程的晶格玻尔兹曼计划。作为形式分析的结果,出现了一个新的渐近偏微分方程--阻尼声学系统。互补的数值实验建立了收敛的标量D2 Q9晶格玻尔兹曼计划与多个弛豫时间和声学缩放在这个特定的情况下的倏逝弛豫对阻尼声学系统的数值解。

英文摘要:

In this work, we study numerically the convergence of the scalar D2Q9 lattice Boltzmann scheme with multiple relaxation times when the time step is proportional to the space step and tends to zero. We do this by a combination of theory and numerical experiment. The classical formal analysis when all the relaxation parameters are fixed and the time step tends to zero shows that the numerical solution converges to solutions of the heat equation, with a constraint connecting the diffusivity, the space step and the coefficient of relaxation of the momentum. If the diffusivity is fixed and the space step tends to zero, the relaxation parameter for the momentum is very small, causing a discrepency between the previous analysis and the numerical results. We propose a new analysis of the method for this specific situation of evanescent relaxation, based on the dispersion equation of the lattice Boltzmann scheme. A new asymptotic partial differential equation, the damped acoustic system, is emergent as a result of this formal analysis. Complementary numerical experiments establish the convergence of the scalar D2Q9 lattice Boltzmann scheme with multiple relaxation times and acoustic scaling in this specific case of evanescent relaxation towards the numerical solution of the damped acoustic system.

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