2014
DOI: 10.1142/s0218202514500158
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A robust and entropy-satisfying numerical scheme for fluid flows in discontinuous nozzles

Abstract: We propose in this work an original finite volume scheme for the system of gas dynamics in a nozzle. Our numerical method is based on a piecewise constant discretization of the crosssection and on a approximate Riemann solver in the sense of Harten, Lax and van Leer. The solver is obtained by the use of a relaxation approximation that leads to a positive and entropy satisfying numerical scheme for all variation of section, even discontinuous with arbitrary large jumps. To do so, we introduce in the first step … Show more

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Cited by 15 publications
(23 citation statements)
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“…In the equality case, the solution is said to be energy-preserving. System (4.33) is nothing but the relaxation system introduced in [17] for the approximation of nozzle flows, and for which the associated Riemann problem has been fully resolved. Hence, we actually calculate a solution W(y, t) of the Riemann problem associated with system (4.33), and the solution for the original Riemann problem (4.20)−(4.21) is obtained by W(x, t) = W(x− u * 2 t, t), and by adding u * 2 to the velocities w 1 .…”
Section: A Convenient Change Of Variablesmentioning
confidence: 99%
See 1 more Smart Citation
“…In the equality case, the solution is said to be energy-preserving. System (4.33) is nothing but the relaxation system introduced in [17] for the approximation of nozzle flows, and for which the associated Riemann problem has been fully resolved. Hence, we actually calculate a solution W(y, t) of the Riemann problem associated with system (4.33), and the solution for the original Riemann problem (4.20)−(4.21) is obtained by W(x, t) = W(x− u * 2 t, t), and by adding u * 2 to the velocities w 1 .…”
Section: A Convenient Change Of Variablesmentioning
confidence: 99%
“…For the resolution, we only consider solutions with the subsonic wave ordering u * 2 < u * 1 since the other possible wave orderings can be obtained by the Galilean invariance of the equations. This ordering for (4.20) corresponds to the wave ordering w 1 − a 1 τ 1 < 0 < w 1 < w 1 + a 1 τ 1 for (4.33), which in [17] is referred to as the < 1, 2 > wave configuration:…”
Section: A Convenient Change Of Variablesmentioning
confidence: 99%
“…Existence and stability results for the shallow water system have been established in [27,21,23,28]. Concerning approximation, many schemes have been proposed, see for example [25,4,3,6,12,7,11,19,20]. The hydrostatic reconstruction scheme and its variants [4,24,18,17,16,15] is often used, and it is the subject of the present paper.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…According to the property (A. 19) we can now define a path v(t) ∈ U m , for 0 ≤ t ≤ 1, connecting the two states U 1 , U 2 satisfying (A.18), by…”
Section: )mentioning
confidence: 99%
“…In particular, condition (F4) may be hard to obtain. One may mention some of them: the non-conservative Godunov scheme [28], a modified kinetic scheme [35], Suliciu's relaxation method [5,13,4], entropy-stable schemes [18]. .…”
Section: An Example Of Well-balanced Schemementioning
confidence: 99%