2019
DOI: 10.1002/fld.4716
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Multistep lattice Boltzmann methods: Theory and applications

Abstract: Summary This paper presents a framework for incorporating arbitrary implicit multistep schemes into the lattice Boltzmann method. While the temporal discretization of the lattice Boltzmann equation is usually derived using a second‐order trapezoidal rule, it appears natural to augment the time discretization by using multistep methods. The effect of incorporating multistep methods into the lattice Boltzmann method is studied in terms of accuracy and stability. Numerical tests for the third‐order accurate Adams… Show more

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Cited by 30 publications
(19 citation statements)
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“…A partial answer can be found in the literature. Indeed, a critical Mach number of approximately 0.73 was observed by Wilde et al [74], by adopting several numerical discretizations of the BGK-DVBE. Hereafter, we will check if this result can be extended to the opposite viewpoint, i.e.…”
Section: Sophisticated Collision Models As a Way To Improve The Linear Stabilitymentioning
confidence: 97%
See 1 more Smart Citation
“…A partial answer can be found in the literature. Indeed, a critical Mach number of approximately 0.73 was observed by Wilde et al [74], by adopting several numerical discretizations of the BGK-DVBE. Hereafter, we will check if this result can be extended to the opposite viewpoint, i.e.…”
Section: Sophisticated Collision Models As a Way To Improve The Linear Stabilitymentioning
confidence: 97%
“…Interestingly, this upper stability limit can be shown to depend on both the lattice and the type of equilibrium (polynomial, entropic, etc.). In addition, it does not seem to be impacted by either the collision model [11,12,76], or the numerical discretization [74].
Figure 4Mach number (Ma) corresponding to the linear stability limit of the D2Q9-BGK-DVBE, for various angles ϕ of the mean flow and ν = 10 −6 .
…”
Section: Linear Stability Analyses Of the Discrete Velocity Boltzmann Equationmentioning
confidence: 99%
“…with the relaxation time τ = ν/(c 2 s δ t ) + 0.5, where the term of 0.5 is a consequence of the second-order time integration in terms of the trapezoidal rule [48][49][50]. The relaxation time τ Pr = (τ − 0.5)/Pr + 0.5 is related to the Prandtl number Pr.…”
Section: Variable Heat Capacity Ratiomentioning
confidence: 99%
“…For the Hermite polynomial formulations, one obtains the upper limit Ma max = √ 3 − 1 ≈ 0.73, with Ma max obtained by considering all possible orientations of the mean flow and keeping the minimal value. Interestingly, one cannot increase this critical Mach number by changing the collision model [43,79] or the numerical scheme [80]. In fact, this can only be achieved by modifying the velocity discretization and the equilibrium state [9,16,43].…”
Section: B Linear Stability Domainmentioning
confidence: 99%