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A volume-preserving sharpening approach for the propagation of sharp phase boundaries in multiphase lattice Boltzmann simulations

机译:在多相晶格玻尔兹曼模拟中传播尖锐相界的保留体积锐化方法

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摘要

Lattice Boltzmann models that recover a macroscopic description of multiphase flow of immiscible liquids typically represent the boundaries between phases using a scalar function, the phase field, that varies smoothly over several grid points. Attempts to tune the model parameters to minimise the widths of these interfaces typically lead to the interfaces becoming fixed to the underlying grid instead of advecting with the fluid velocity. This phenomenon, known as lattice pinning, is strikingly similar to that associated with the numerical simulation of conservation laws coupled to stiff algebraic source terms. We present a lattice Boltzmann formulation of the model problem proposed by LeVeque and Yee (1990) [3] to study the latter phenomenon in the context of computational combustion, and offer a volume-conserving extension in multiple space dimensions. Inspired by the random projection method of Bao and Jin (2000) [1] we further generalise this formulation by introducing a uniformly distributed quasi-random variable into the term responsible for the sharpening of phase boundaries. This method is mass conserving, gives correct average propagation speeds over many timesteps, and is shown to significantly delay the onset of pinning as the interface width is reduced. © 2010 Elsevier Ltd.
机译:恢复对不混溶液体的多相流进行宏观描述的莱迪思·博尔兹曼(Lattice Boltzmann)模型通常使用标量函数(相场)表示相之间的边界,该标量函数在多个网格点上平滑变化。尝试调整模型参数以最小化这些界面的宽度通常会导致界面变得固定在基础网格上,而不是随流体速度平移。这种现象称为晶格固定,与与刚性代数源项耦合的守恒定律的数值模拟相关的现象极为相似。我们提出由LeVeque和Yee(1990)提出的模型问题的格子Boltzmann公式[3],以研究在计算燃烧的情况下的后一种现象,并在多个空间维度上提供体积守恒的扩展。受到Bao and Jin(2000)[1]的随机投影方法的启发,我们通过将均匀分布的准随机变量引入负责相位边界锐化的术语来进一步推广该公式。该方法节省了质量,在许多时间步长上都提供了正确的平均传播速度,并且随着界面宽度的减小,该方法显着延迟了钉扎的开始。 ©2010爱思唯尔有限公司。

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    Reis, T; Dellar, PJ;

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  • 年度 2011
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  • 原文格式 PDF
  • 正文语种 eng
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