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A pseudopotential multiphase lattice Boltzmann model based on high-order difference

机译:基于高阶差分的伪势多相晶格玻尔兹曼模型

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摘要

The hyperbolic tangent function is usually used as a reliable approximation of the equilibrium density distributions of a system with phase transitions. However, analyzing the accuracies of the numerical derivatives, we find that its numerical derivatives computed by central difference method (CDM) may deviate significantly from its analytical solutions, while those computed by high-order difference method (HDM) can agree very well. Therefore, we introduce HDM to evaluate the interparticle interactions instead of popular CDM, and propose a pseudopotential multiphase lattice Boltzmann model based on high-order difference method. The present model not only retains the advantages of the pseudopotential model, such as easy implementation, high efficiency, full parallelism and so on, but also achieves higher accuracies. To verify the performances of this model, several multiphase flow simulations are conducted, including both stationary and dynamic situations. Firstly, full thermodynamic consistencies for the popular equations of state have been achieved in large temperature range and at large density ratio, without any combining interaction and any additional adjustable parameter of interaction. Secondly, with highorder difference, either the interparticle interaction proposed by Shan-Chen or by Zhang-Chen can equally depict the phase transitions of the fluids with all selected equations of the state. These numerical agreements based on HDM are consistent to the theoretical analysis that the two interactions are mathematically identical. Thirdly, the present model is stable and can be easily applied to various practical simulations and expected to obtain some more interesting results. (C) 2018 Elsevier Ltd. All rights reserved.
机译:双曲正切函数通常用作具有相变的系统的平衡密度分布的可靠近似。但是,通过分析数值导数的精度,我们发现通过中央差分法(CDM)计算的数值导数可能与其解析解有很大出入,而通过高阶差分法(HDM)计算的数值导数可以很好地吻合。因此,我们引入了HDM而不是流行的CDM来评估粒子间的相互作用,并提出了一种基于高阶差分法的伪势多相晶格Boltzmann模型。本模型不仅保留了伪电位模型的优点,例如易于实现,高效,完全并行等优点,而且具有较高的准确性。为了验证该模型的性能,进行了多个多相流模拟,包括静态和动态情况。首先,在较大的温度范围和较大的密度比下,无需任何组合相互作用和任何附加的可调相互作用参数,即可获得流行状态方程的完全热力学一致性。其次,由于存在高阶差异,Shan-Chen或Zhang-Chen提出的粒子间相互作用可以用所有选定的状态方程式相等地描述流体的相变。这些基于HDM的数值协议与理论分析一致,即两个相互作用在数学上是相同的。第三,本模型是稳定的,可以容易地应用于各种实际仿真中,并有望获得更多有趣的结果。 (C)2018 Elsevier Ltd.保留所有权利。

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