1999
DOI: 10.1103/physreve.60.464
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Rayleigh-Bénard simulation using the gas-kinetic Bhatnagar-Gross-Krook scheme in the incompressible limit

Abstract: In this paper, a gas-kinetic Bhatnagar-Gross-Krook ͑BGK͒ model is constructed for the Rayleigh-Bénard thermal convection in the incompressible flow limit, where the flow field and temperature field are described by two coupled BGK models. Since the collision times in the corresponding BGK models can be different, the Prandtl number can be changed to any value instead of a fixed Prϭ1 in the original BGK model ͓P. L. Bhatnagar, E. P. Gross, and M. Krook, Phys. Rev. 94, 511 ͑1954͔͒. The two-dimensional Rayleigh-B… Show more

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Cited by 36 publications
(27 citation statements)
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“…The ideal equation of state used in most compressible code will automatically generate a large density change if there are significant temperature variations. This related issue is discussed in [13].…”
Section: Resultsmentioning
confidence: 99%
“…The ideal equation of state used in most compressible code will automatically generate a large density change if there are significant temperature variations. This related issue is discussed in [13].…”
Section: Resultsmentioning
confidence: 99%
“…Among these methods, the LBE and GKS methods are specifically designed as numerical methods for CFD: the former is only valid for near incompressible flows while the latter is for fully compressible flows. Both methods have been applied to simulate viscous flows [3,4], heat transfer problems [5,6], shallow water equations [7], multiphase [8][9][10][11] and multi-component [12][13][14][15][16][17] flows, magnetohydrodynamics [18][19][20], and microflows [21][22][23][24]. Besides their common connections to the Boltzmann equation, the LBE and GKS methods are quite different in many ways.…”
Section: Introductionmentioning
confidence: 98%
“…This makes the expression of numerical fluxes be hardly given explicitly for the Maxwellian function–based GKS. Fortunately, for simulation of incompressible flows, this kind of method can be simplified to some extent as the flow variables change smoothly in the domain . In the work of Su et al, the compressible GKS is directly extended to simulate incompressible flows by using the third‐order accurate interpolation scheme to compute the macroscopic variables and their slopes at the cell interface.…”
Section: Introductionmentioning
confidence: 99%