2022
DOI: 10.1016/j.jcp.2021.110858
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Hydrodynamic limits and numerical errors of isothermal lattice Boltzmann schemes

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Cited by 18 publications
(8 citation statements)
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References 87 publications
(285 reference statements)
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“…The enthalpy equation ( 4) is solved at the same time using a finite difference discretization under the non-conservative form, exactly as presented by Tayyab et al [36,37]. Second-order consistency to the macroscopic equations (1-4) can be shown via Chapman-Enskog [52], or Taylor [53,54] expansions.…”
Section: Lbm Description For Low-mach Number Approximationmentioning
confidence: 99%
“…The enthalpy equation ( 4) is solved at the same time using a finite difference discretization under the non-conservative form, exactly as presented by Tayyab et al [36,37]. Second-order consistency to the macroscopic equations (1-4) can be shown via Chapman-Enskog [52], or Taylor [53,54] expansions.…”
Section: Lbm Description For Low-mach Number Approximationmentioning
confidence: 99%
“…Note that (11) is not exactly the Perona-Malik Equation (1) but one can demonstrate that its properties are very similar to (1). First, one needs to introduce an orthonormal frame consisting of two vectors: one vector defined by T is parallel to ∇I and another one N is perpendicular to ∇I.…”
Section: Lattice Boltzmann Scheme For Nonlinear Diffusionmentioning
confidence: 99%
“…Although one can take large time steps while modeling a diffusion process using conventional LB models, the limitations emerge from accuracy issues. For non-small values of the time step and diffusion coefficient, LB models suffer from hyper-viscous errors (or truncation errors) [7][8][9][10][11][12]. In order to improve the accuracy of LB schemes, several approaches can be adopted.…”
Section: Introductionmentioning
confidence: 99%
“…Given (i) the excellent dissipation properties of LBM for acoustic propagation [26], including for hybrid methods [12,13] for which vortical and acoustic mode propagations are convected by the LBM scheme [27][28][29] while species/entropy modes are convected with a specifically designed scheme [30,31] ; and (ii) the success encountered in simulating burners with complex geometries [23,25] for a reasonable cost, the next logical step is to investigate and develop LBM able to model thermo-acoustic instabilities.…”
Section: Introductionmentioning
confidence: 99%