Body-force modelling in thermal compressible flows with the lattice Boltzmann method
Body-force modelling in the lattice Boltzmann method (LBM) has been studied extensively in the incompressible limit but rarely discussed for thermal compressible flows. Here we present a systematic approach of incorporating body force in the LBM which is valid for thermal compressible and non-equilibrium flows. In particular, a LBM forcing scheme accurate for the energy equation with second-order time accuracy is given. New and essential in this scheme is the third-moment contribution of the force term. It is shown via Chapman-Enskog analysis that the absence of this contribution causes an erroneous heat flux quadratic in Mach number and linear in temperature variation. The theoretical findings are verified and the necessity of the third-moment contribution is demonstrated by numerical simulations.
National Natural Science Foundation of China grant ; Dept. of Science and Technology of Guangdong Province grant[2020B1212030001] ; Shenzhen Science and Technology Program grant[KQTD20180411143441009]
|WOS Research Area|
Mechanics ; Physics
Mechanics ; Physics, Fluids & Plasmas
|WOS Accession No|
|ESI Research Field|
Cited Times [WOS]:1
|Document Type||Journal Article|
|Department||Department of Mechanics and Aerospace Engineering|
Department of Mechanics and Aerospace Engineering,Southern University of Science and Technology,Shenzhen,518055,China
|First Author Affilication||Department of Mechanics and Aerospace Engineering|
|First Author's First Affilication||Department of Mechanics and Aerospace Engineering|
Li，Zuoxu,Shan，Xiaowen. Body-force modelling in thermal compressible flows with the lattice Boltzmann method[J]. Journal of Fluid Mechanics,2023,964.
Li，Zuoxu,&Shan，Xiaowen.(2023).Body-force modelling in thermal compressible flows with the lattice Boltzmann method.Journal of Fluid Mechanics,964.
Li，Zuoxu,et al."Body-force modelling in thermal compressible flows with the lattice Boltzmann method".Journal of Fluid Mechanics 964(2023).
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