All Mach Number Second Order Semi-implicit Scheme for the Euler Equations of Gas Dynamics

被引:62
作者
Boscarino, S. [1 ]
Russo, G. [1 ]
Scandurra, L. [2 ]
机构
[1] Univ Catania, Dept Math & Comp Sci, Viale A Doria 6, I-95125 Catania, Italy
[2] Heinrich Heine Univ Dusseldorf, Dusseldorf, North Rhine Wes, Germany
基金
欧盟地平线“2020”;
关键词
All Mach number; Asymptotic preserving; Staggered grid; Isentropic Euler equations; Compressible flow; Incompressible limit; Semi-implicit schemes; IMEX methods; Runge Kutta methods; RUNGE-KUTTA SCHEMES; PRESERVING AP SCHEMES; HYPERBOLIC SYSTEMS; INCOMPRESSIBLE-FLOW; SPEED; EXTENSION;
D O I
10.1007/s10915-018-0731-9
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
This paper presents an asymptotic preserving (AP) all Mach number finite volume shock capturing method for the numerical solution of compressible Euler equations of gas dynamics. Both isentropic and full Euler equations are considered. The equations are discretized on a staggered grid. This simplifies flux computation and guarantees a natural central discretization in the low Mach limit, thus dramatically reducing the excessive numerical diffusion of upwind discretizations. Furthermore, second order accuracy in space is automatically guaranteed. For the time discretization we adopt an Semi-IMplicit/EXplicit (S-IMEX) discretization getting an elliptic equation for the pressure in the isentropic case and for the energy in the full Euler case. Such equations can be solved linearly so that we do not need any iterative solver thus reducing computational cost. Second order in time is obtained by a suitable S-IMEX strategy taken from Boscarino et al. (J Sci Comput 68:975-1001, 2016). Moreover, the CFL stability condition is independent of the Mach number and depends essentially on the fluid velocity. Numerical tests are displayed in one and two dimensions to demonstrate performance of our scheme in both compressible and incompressible regimes.
引用
收藏
页码:850 / 884
页数:35
相关论文
共 49 条
[1]  
[Anonymous], SIAM J SCI COMPUT
[2]  
[Anonymous], 348 IGPM RWTH AACH
[3]  
[Anonymous], LINEARLY IMPLI UNPUB
[4]  
[Anonymous], ARXIV09081929
[5]  
[Anonymous], THESIS
[6]  
[Anonymous], HIGH ORDER SEM UNPUB
[7]  
[Anonymous], 2002, FINITE VOLUME METHOD
[8]  
Arminjon P, 1998, INT J COMPUT FLUID D, V9, pI
[9]   Implicit-explicit Runge-Kutta methods for time-dependent partial differential equations [J].
Ascher, UM ;
Ruuth, SJ ;
Spiteri, RJ .
APPLIED NUMERICAL MATHEMATICS, 1997, 25 (2-3) :151-167
[10]   IMPLICIT-EXPLICIT RUNGE-KUTTA SCHEMES FOR HYPERBOLIC SYSTEMS AND KINETIC EQUATIONS IN THE DIFFUSION LIMIT [J].
Boscarino, S. ;
Pareschi, L. ;
Russo, G. .
SIAM JOURNAL ON SCIENTIFIC COMPUTING, 2013, 35 (01) :A22-A51