On Lattice Boltzmann Methods based on vector-kinetic models for hyperbolic partial differential equations

Megala Anandan, S. V. Raghurama Rao
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Abstract

In this paper, we are concerned about the lattice Boltzmann methods (LBMs) based on vector-kinetic models for hyperbolic partial differential equations. In addition to usual lattice Boltzmann equation (LBE) derived by explicit discretisation of vector-kinetic equation (VKE), we also consider LBE derived by semi-implicit discretisation of VKE and compare the relaxation factors of both. We study the properties such as H-inequality, total variation boundedness and positivity of both the LBEs, and infer that the LBE due to semi-implicit discretisation naturally satisfies all the properties while the LBE due to explicit discretisation requires more restrictive condition on relaxation factor compared to the usual condition obtained from Chapman-Enskog expansion. We also derive the macroscopic finite difference form of the LBEs, and utilise it to establish the consistency of LBEs with the hyperbolic system. Further, we extend this LBM framework to hyperbolic conservation laws with source terms, such that there is no spurious numerical convection due to imbalance between convection and source terms. We also present a D$2$Q$9$ model that allows upwinding even along diagonal directions in addition to the usual upwinding along coordinate directions. The different aspects of the results are validated numerically on standard benchmark problems.
基于双曲偏微分方程向量动力学模型的格点玻尔兹曼方法
本文关注基于双曲偏微分方程矢量动力学模型的晶格玻尔兹曼方法(LBM)。除了通过矢量动力学方程(VKE)的显式离散化导出的通常晶格玻尔兹曼方程(LBE)之外,我们还考虑了通过 VKE 的半隐式离散化导出的 LBE,并比较了两者的弛豫因子。我们研究了两种 LBE 的 H-inequality、总变异有界性和正性等性质,并推断出半隐式离散化的 LBE 自然满足所有性质,而显式离散化的 LBE 与 Chapman-Enskog 扩展得到的通常条件相比,对松弛因子要求更严格。此外,我们将这一 LBM 框架扩展到具有源项的双曲守恒定律,这样就不会由于对流和源项间的不平衡而产生虚假的数值对流。我们还提出了一个 D$2$Q$9$ 模型,除了通常的沿坐标方向上卷之外,还允许沿对角线方向上卷。在标准基准问题上对结果的不同方面进行了数值验证。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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