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晶格动力学格式的稳定性及自由弛豫参数的选择

Stability of the lattice kinetic scheme and choice of the free relaxation parameter.

作者信息

Hosseini S A, Coreixas C, Darabiha N, Thévenin D

机构信息

Laboratory of Fluid Dynamics and Technical Flows, University of Magdeburg "Otto von Guericke," D-39106 Magdeburg, Germany.

Laboratoire EM2C, CNRS, CentraleSupélec, Université Paris-Saclay, 3 rue Joliot Curie, 91192, Gif-sur-Yvette Cedex, France.

出版信息

Phys Rev E. 2019 Jun;99(6-1):063305. doi: 10.1103/PhysRevE.99.063305.

Abstract

The lattice kinetic scheme (LKS), a modified version of the classical single relaxation time (SRT) lattice Boltzmann method, was initially developed as a suitable numerical approach for non-Newtonian flow simulations and a way to reduce memory consumption of the original SRT approach. The better performances observed for non-Newtonian flows are mainly due to the additional degree of freedom allowing an independent control over the relaxation of higher-order moments, independently from the fluid viscosity. Although widely applied to fluid flow simulations, no theoretical analysis of LKS has been performed. The present work focuses on a systematic von Neumann analysis of the linearized collision operator. Thanks to this analysis, the effects of the modified collision operator on the stability domain and spectral behavior of the scheme are clarified. Results obtained in this study show that correct choices of the "second relaxation coefficient" lead, to a certain extent, to a more consistent dispersion and dissipation for large values of the first relaxation coefficient. Furthermore, appropriate values of this parameter can lead to a larger linear stability domain. At moderate and low values of viscosity, larger values of the free parameter are observed to increase dissipation of kinetic modes, while leaving the acoustic modes untouched and having a less pronounced effect on the convective mode. This increased dissipation leads in general to less pronounced sources of nonlinear instability, thus improving the stability of the LKS.

摘要

格子动力学格式(LKS)是经典单松弛时间(SRT)格子玻尔兹曼方法的一种改进形式,最初被开发为一种适用于非牛顿流模拟的数值方法,也是一种减少原始SRT方法内存消耗的途径。在非牛顿流中观察到的更好性能主要归因于额外的自由度,它允许独立控制高阶矩的松弛,而与流体粘度无关。尽管LKS已广泛应用于流体流动模拟,但尚未对其进行理论分析。目前的工作重点是对线性化碰撞算子进行系统的冯·诺依曼分析。通过该分析,阐明了修正后的碰撞算子对格式的稳定域和谱行为的影响。本研究获得的结果表明,“第二松弛系数”的正确选择在一定程度上会使第一松弛系数较大时的色散和耗散更加一致。此外,该参数的适当值可导致更大的线性稳定域。在中等和低粘度值下,观察到自由参数的较大值会增加动力学模式的耗散,同时不影响声学模式,并且对对流模式的影响较小。这种增加的耗散通常会导致非线性不稳定源不太明显,从而提高LKS的稳定性。

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