2010
DOI: 10.1016/j.jcp.2009.09.044
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Analysis of Godunov type schemes applied to the compressible Euler system at low Mach number

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Cited by 179 publications
(350 citation statements)
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“…As a consequence, there are two different time scales in the compressible NavierStokes system used to model the flow in the nuclear core: a first time scale which is the material time scale t mat and a second time scale which is the acoustic time scale t ac . Since t ac t mat and since the usefull time scale is t mat in the study of thermal-hydraulic phenomena in a nuclear core whose the flow is at low Mach number, the discretization of the compressible Navier-Stokes system needs to use an implicit scheme in such a way that the time step is of the order or greater than t mat , implicit scheme which may be expensive from a CPU point of view and which may suffer from a lack of robustness and/or of a lack of accuracy [6,10].…”
Section: Introductionmentioning
confidence: 99%
“…As a consequence, there are two different time scales in the compressible NavierStokes system used to model the flow in the nuclear core: a first time scale which is the material time scale t mat and a second time scale which is the acoustic time scale t ac . Since t ac t mat and since the usefull time scale is t mat in the study of thermal-hydraulic phenomena in a nuclear core whose the flow is at low Mach number, the discretization of the compressible Navier-Stokes system needs to use an implicit scheme in such a way that the time step is of the order or greater than t mat , implicit scheme which may be expensive from a CPU point of view and which may suffer from a lack of robustness and/or of a lack of accuracy [6,10].…”
Section: Introductionmentioning
confidence: 99%
“…The scheme was shown to be L 2 stable under a suitable CFL condition. The proofs extend the ideas introduced in [5] for the study of the homogeneous wave equations in low Mach number regimes. In this paper, our objective is to study in the same context the numerical scheme introduced in [3] as a well-balanced (WB) scheme for the Shallow Water equations with Coriolis source term (1).…”
Section: Introductionmentioning
confidence: 71%
“…It requires adjustments to solve for 2D or 3D flows, at low Mach number, on a cartesian mesh. As Mach number goes to zero, in some extreme 2D or 3D cases, the native method does converge but the solution is not consistent with the analytical or experimental solution [4]. A so-called "pressure correction" is added to the initial solver to solve for the right physical solution.…”
Section: Introductionmentioning
confidence: 99%
“…Le schéma numérique du code FLICA4 est basé sur une technique de volumes finis où les flux numériques convectifs sont calculésà l'aide d'un solveur colocalisé appelé Roe [3]. L'analyse de cette méthode numérique montre qu'à bas nombre de Mach, il est nécessaire d'introduire des modifications spécifiques aux géométries 2D ou 3D sur un maillage cartésien sans quoi la solution ne converge pas vers la bonne solution lorsque le nombre de Mach tend vers zéro [4]. C'est la raison pour laquelle une correction dite "correction de pression" est appliquée.…”
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