2010
DOI: 10.1016/j.cpc.2010.06.004
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Finite-difference stable stencils based on least-square quadric fitting

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Cited by 5 publications
(6 citation statements)
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“…The SS stencil was verified to have stability while solving an ill-posed problem such as the anti-diffusion equation, and it has been tested stably in various cases, showing second-order accuracy as well [32]. Here, as what is implemented by Dupuy et al, we use the SS stencil to discretize the Laplacian term ∇ 2 T in the sub-operator equation L 2 :…”
Section: Temperature Fieldmentioning
confidence: 98%
See 1 more Smart Citation
“…The SS stencil was verified to have stability while solving an ill-posed problem such as the anti-diffusion equation, and it has been tested stably in various cases, showing second-order accuracy as well [32]. Here, as what is implemented by Dupuy et al, we use the SS stencil to discretize the Laplacian term ∇ 2 T in the sub-operator equation L 2 :…”
Section: Temperature Fieldmentioning
confidence: 98%
“…Shu et al [31] has integrated LBM with FSM to simulate the high Reynolds number flow, but its splitting is ill-posed and without rigorous analysis, its accuracy, consistency and stability are not established. In our model the PS-TLBM is combined with the second-order Strang operator splitting method and SS finite difference scheme [32] in favor of better numerical stability.…”
Section: Introductionmentioning
confidence: 99%
“…In detail, as the LBM has optimal stability with the relaxation time of 1.0 (Sterling and Chen, 1996; Zhao, 2013), α 0 is accordingly set to be cs2δt(10.5). Other than ordinary central difference scheme, we use the SS stencil (Dupuy et al , 2010) to discretize the Laplacian term in the sub-operator equation L 2 : …”
Section: Lattice Boltzmann Implementationmentioning
confidence: 99%
“…In the present work we are only interested in studying the momentum exchange, thus we provide only information on the pressure and momentum distribution modeled with Here f t i,x is the ith density function (or pseudoparticle) in node x at time t, and e i the discrete velocity vector of the pseudoparticle i. The collision term, Ω i , and the forcing terms, F i , are widely used in lattice Boltzmann schemes for modifying or adding extra terms to the equation system (1)- (3). Different expressions can be used for these source terms [7,12].…”
Section: The Lattice Boltzmann Modelmentioning
confidence: 99%
“…We use a first-order explicit in time finite difference technique for solving equation (16). The solution with two different stencils are studied, namely central differences (C) and a so-called stable stencil based on a least squares quadric fitting [3] for antidiffusion problems (SS). This last family of stencils computes correctly the actual curvature of the surfaces and at the same time counteracts the formation of ripples of a wavelength of two lattice units.…”
Section: Finite Difference Schemementioning
confidence: 99%