Rectangular Lattice Boltzmann Equation for Gaseous Microscale Flow

被引:9
作者
Ren, Junjie [1 ]
Guo, Ping [2 ]
Guo, Zhaoli [3 ]
机构
[1] Southwest Petr Univ, Sch Sci, Chengdu 610500, Peoples R China
[2] Southwest Petr Univ, State Key Lab Oil & Gas Reservoir Geol & Exploita, Chengdu 610500, Peoples R China
[3] Huazhong Univ Sci & Technol, State Key Lab Coal Combust, Wuhan 430074, Peoples R China
基金
中国国家自然科学基金;
关键词
Lattice Boltzmann equation; gaseous microscale flow; rectangular lattice; boundary conditions; multiple-relaxation time; BOUNDARY-CONDITIONS; MICROCHANNEL FLOWS; FLUID-FLOWS; GAS-FLOWS; CONTRACTION; SIMULATION; EXPANSION; REGIME; MEMS;
D O I
10.4208/aamm.2014.m672
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
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 multiple-relaxation-time (MRT) collision operator, i.e., the combined bounce-back/specular-reflection (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 not equal 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.
引用
收藏
页码:306 / 330
页数:25
相关论文
共 37 条
[1]   Simulation of gas flow in microchannels with a sudden expansion or contraction [J].
Agrawal, A ;
Djenidi, L ;
Antonia, RA .
JOURNAL OF FLUID MECHANICS, 2005, 530 :135-144
[2]   Lattice-Boltzmann Method for Complex Flows [J].
Aidun, Cyrus K. ;
Clausen, Jonathan R. .
ANNUAL REVIEW OF FLUID MECHANICS, 2010, 42 :439-472
[3]   Kinetic boundary conditions in the lattice Boltzmann method [J].
Ansumali, S ;
Karlin, IV .
PHYSICAL REVIEW E, 2002, 66 (02) :1-026311
[4]   Lattice Boltzmann equation on a two-dimensional rectangular grid [J].
Bouzidi, M ;
d'Humières, D ;
Lallemand, P ;
Luo, LS .
JOURNAL OF COMPUTATIONAL PHYSICS, 2001, 172 (02) :704-717
[5]  
Cercignani C., 1990, Mathematical Methods in Kinetic Theory
[6]   Effect of the forcing term in the multiple-relaxation-time lattice Boltzmann equation on the shear stress or the strain rate tensor [J].
Chai, Zhenhua ;
Zhao, T. S. .
PHYSICAL REVIEW E, 2012, 86 (01)
[7]   Comment on "Rectangular lattice Boltzmann method" [J].
Chikatamarla, Shyam ;
Karlin, Ilya .
PHYSICAL REVIEW E, 2011, 83 (04)
[8]   Two relaxation time lattice Boltzmann model for rarefied gas flows [J].
Esfahani, Javad Abolfazli ;
Norouzi, Ali .
PHYSICA A-STATISTICAL MECHANICS AND ITS APPLICATIONS, 2014, 393 :51-61
[9]   Discrete effects on boundary conditions for the lattice Boltzmann equation in simulating microscale gas flows [J].
Guo, Zhaoli ;
Shi, Baochang ;
Zhao, T. S. ;
Zheng, Chuguang .
PHYSICAL REVIEW E, 2007, 76 (05)
[10]   Lattice Boltzmann equation with multiple effective relaxation times for gaseous microscale flow [J].
Guo, Zhaoli ;
Zheng, Chuguang ;
Shi, Baochang .
PHYSICAL REVIEW E, 2008, 77 (03)