Abstract

The computation of compressible flows at all Mach numbers is a very challenging problem. An efficient numerical method for solving this problem needs to have shock-capturing capability in the high Mach number regime, while it can deal with stiffness and accuracy in the low Mach number regime. This paper designs a high order semi-implicit weighted compact nonlinear scheme (WCNS) for the all-Mach isentropic Euler system of compressible gas dynamics. To avoid severe Courant-Friedrichs-Levy (CFL) restrictions for low Mach flows, the nonlinear fluxes in the Euler equations are split into stiff and non-stiff components. A third-order implicit-explicit (IMEX) method is used for the time discretization of the split components and a fifth-order WCNS is used for the spatial discretization of flux derivatives. The high order IMEX method is asymptotic preserving and asymptotically accurate in the zero Mach number limit. One- and two-dimensional numerical examples in both compressible and incompressible regimes are given to demonstrate the advantages of the designed IMEX WCNS.

Highlights

  • Low-Mach number flows in fluid dynamics that are slow compared with the speed of sound can be described by the following scaled isentropic Euler equations.ρt + ∇ · = 0,t +∇ · + 1 ε2 ∇ p = (1)where ρ(x, t) > 0, u(x, t) = (u(x, t), v(x, t)) and q = ρu(x, t) are the density, velocity and momentum of the fluid, respectively, and ε > 0 is the scaled Mach number that is a measure of compressibility of the fluid

  • 3 IMEX method we briefly describe the framework of IMEX time discretization designed for the numerical integration of the stiff ordinary differential equation (ODE) as follows

  • 7 Conclusions In this work, we have designed a high order IMEX weighted compact nonlinear scheme (WCNS) for the compressibleincompressible limit problems described as scaled isentropic Euler equations

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Summary

Introduction

In view of the good performance of the IMEX time discretization method and the WCNS’s, we design a high order IMEX WCNS for the all-Mach isentropic Euler system based on the acoustic/advection splitting strategy [10]. Remark 3 To update the solutions from tn to tn+1 by the pth-order IMEX-ARSp WCNS, we first solve the elliptic equation (33) to obtain ρ(k) and calculate explicitly q(k) using (36). The IMEX-ARSp scheme is asymptotically stable with the time-step restrictions (38) or (39) independent of the Mach number ε.

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