2013
DOI: 10.1016/j.compfluid.2013.07.010
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Random sampling remap for compressible two-phase flows

Abstract: International audienceIn this paper, we address the problem of solving accurately gas-liquid compressible flows, without pressure oscillations at the gas-liquid interface. We introduce a new Lagrange-projection scheme based on a random sampling technique of Chalons and Goatin. We compare it to a Ghost Fluid approach introduced previously. Despite the non-conservative feature of the schemes, we observe the numerical convergence towards the relevant weak solution, for shock-contact interaction test cases. Finall… Show more

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Cited by 15 publications
(19 citation statements)
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“…The method was first proposed in [6] for a particular traffic flow model. It does not introduce a mixture zone and extends the one-dimensional method described in [2]. More precisely, we construct a numerical scheme that preserves the hyperbolic domain without diffusion H,…”
mentioning
confidence: 99%
“…The method was first proposed in [6] for a particular traffic flow model. It does not introduce a mixture zone and extends the one-dimensional method described in [2]. More precisely, we construct a numerical scheme that preserves the hyperbolic domain without diffusion H,…”
mentioning
confidence: 99%
“…Finally Colella had improved the method of Chorin in [30,31], especially by introducing the so-called van der Corput pseudo-random sequence. The technique has been widely used for hyperbolic problems which exhibit sharp discontinuities: in [32] for nonconservative hyperbolic problems for compressible materials, in [33,34] for traffic flow models, in [35] for compressible fluid-particule interaction or in [36,37] for the simulation of two-fluid flows.…”
Section: Introductionmentioning
confidence: 99%
“…initial data for which the quantities ϕ, s, Q, H are constant); • for a flow in a duct with constant cross-section ducts, it computes exactly the contact discontinuities, with no smearing at the interface; • if at the initial time the mass fraction is in {0, 1}, then this property is exactly preserved at any time. For detailed proofs, we refer to [1,6]. Some other subtleties are given in the same references.…”
Section: Properties Of the Schemementioning
confidence: 99%
“…We construct a sequence of pseudo-random numbers ω n ∈ [0, 1[. In practice, we consider the (5, 3) van der Corput sequence [1]. According to this number we take…”
Section: Glimm Remapmentioning
confidence: 99%
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