Volume 8, Issue 2
Rectangular Lattice Boltzmann Equation for Gaseous Microscale Flow

Junjie Ren, Ping Guo & Zhaoli Guo

Adv. Appl. Math. Mech., 8 (2016), pp. 306-330.

Published online: 2018-05

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  • Abstract

The lattice Boltzmann equation (LBE) is considered as a promising approach for simulating flows of liquid and gas. Most of LBE studies have been devoted to regular square LBE and few works have focused on the rectangular LBE in the simulation of gaseous microscale flows. In fact, the rectangular LBE, as an alternative and efficient method, has some advantages over the square LBE in simulating flows with certain computational domains of large aspect ratio (e.g., long micro channels). Therefore, in this paper we expand the application scopes of the rectangular LBE to gaseous microscale flow. The kinetic boundary conditions for the rectangular LBE with a multiplerelaxation-time (MRT) collision operator, i.e., the combined bounce-back/specularreflection (CBBSR) boundary condition and the discrete Maxwell’s diffuse-reflection (DMDR) boundary condition, are studied in detail. We observe some discrete effects in both the CBBSR and DMDR boundary conditions for the rectangular LBE and present a reasonable approach to overcome these discrete effects in the two boundary conditions. It is found that the DMDR boundary condition for the square MRT-LBE can not realize the real fully diffusive boundary condition, while the DMDR boundary condition for the rectangular MRT-LBE with the grid aspect ratio a ̸=1 can do it well. Some numerical tests are implemented to validate the presented theoretical analysis. In addition, the computational efficiency and relative difference between the rectangular LBE and the square LBE are analyzed in detail. The rectangular LBE is found to be an efficient method for simulating the gaseous microscale flows in domains with large aspect ratios.

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@Article{AAMM-8-306, author = {Junjie Ren, Ping Guo and Zhaoli Guo}, title = {Rectangular Lattice Boltzmann Equation for Gaseous Microscale Flow}, journal = {Advances in Applied Mathematics and Mechanics}, year = {2018}, volume = {8}, number = {2}, pages = {306--330}, abstract = {

The lattice Boltzmann equation (LBE) is considered as a promising approach for simulating flows of liquid and gas. Most of LBE studies have been devoted to regular square LBE and few works have focused on the rectangular LBE in the simulation of gaseous microscale flows. In fact, the rectangular LBE, as an alternative and efficient method, has some advantages over the square LBE in simulating flows with certain computational domains of large aspect ratio (e.g., long micro channels). Therefore, in this paper we expand the application scopes of the rectangular LBE to gaseous microscale flow. The kinetic boundary conditions for the rectangular LBE with a multiplerelaxation-time (MRT) collision operator, i.e., the combined bounce-back/specularreflection (CBBSR) boundary condition and the discrete Maxwell’s diffuse-reflection (DMDR) boundary condition, are studied in detail. We observe some discrete effects in both the CBBSR and DMDR boundary conditions for the rectangular LBE and present a reasonable approach to overcome these discrete effects in the two boundary conditions. It is found that the DMDR boundary condition for the square MRT-LBE can not realize the real fully diffusive boundary condition, while the DMDR boundary condition for the rectangular MRT-LBE with the grid aspect ratio a ̸=1 can do it well. Some numerical tests are implemented to validate the presented theoretical analysis. In addition, the computational efficiency and relative difference between the rectangular LBE and the square LBE are analyzed in detail. The rectangular LBE is found to be an efficient method for simulating the gaseous microscale flows in domains with large aspect ratios.

}, issn = {2075-1354}, doi = {https://doi.org/10.4208/aamm.2014.m672}, url = {http://global-sci.org/intro/article_detail/aamm/12091.html} }
TY - JOUR T1 - Rectangular Lattice Boltzmann Equation for Gaseous Microscale Flow AU - Junjie Ren, Ping Guo & Zhaoli Guo JO - Advances in Applied Mathematics and Mechanics VL - 2 SP - 306 EP - 330 PY - 2018 DA - 2018/05 SN - 8 DO - http://dor.org/10.4208/aamm.2014.m672 UR - https://global-sci.org/intro/aamm/12091.html KW - AB -

The lattice Boltzmann equation (LBE) is considered as a promising approach for simulating flows of liquid and gas. Most of LBE studies have been devoted to regular square LBE and few works have focused on the rectangular LBE in the simulation of gaseous microscale flows. In fact, the rectangular LBE, as an alternative and efficient method, has some advantages over the square LBE in simulating flows with certain computational domains of large aspect ratio (e.g., long micro channels). Therefore, in this paper we expand the application scopes of the rectangular LBE to gaseous microscale flow. The kinetic boundary conditions for the rectangular LBE with a multiplerelaxation-time (MRT) collision operator, i.e., the combined bounce-back/specularreflection (CBBSR) boundary condition and the discrete Maxwell’s diffuse-reflection (DMDR) boundary condition, are studied in detail. We observe some discrete effects in both the CBBSR and DMDR boundary conditions for the rectangular LBE and present a reasonable approach to overcome these discrete effects in the two boundary conditions. It is found that the DMDR boundary condition for the square MRT-LBE can not realize the real fully diffusive boundary condition, while the DMDR boundary condition for the rectangular MRT-LBE with the grid aspect ratio a ̸=1 can do it well. Some numerical tests are implemented to validate the presented theoretical analysis. In addition, the computational efficiency and relative difference between the rectangular LBE and the square LBE are analyzed in detail. The rectangular LBE is found to be an efficient method for simulating the gaseous microscale flows in domains with large aspect ratios.

Junjie Ren, Ping Guo & Zhaoli Guo. (1970). Rectangular Lattice Boltzmann Equation for Gaseous Microscale Flow. Advances in Applied Mathematics and Mechanics. 8 (2). 306-330. doi:10.4208/aamm.2014.m672
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