A Second-Order Relaxation Flux Solver for Compressible Navier-Stokes Equations based on Generalized Riemann Problem Method
Tuowei Chen, Zhifang Du
TL;DR
The paper develops a Lax-Wendroff-type, second-order flux solver for the 2-D compressible Navier-Stokes equations by embedding a hyperbolic relaxation formulation into a generalized Riemann problem framework. Stiff viscous terms are handled implicitly through GRP-based time derivatives, enabling a standard Euler-like CFL condition and solving a sparse linear system once per time step. Local interface definitions of the relaxation parameters $a$ and $\epsilon$ enhance robustness across smooth and shocked regions, while avoiding explicit evolution of relaxation variables. Extensive inviscid and viscous test cases demonstrate high-resolution performance, accuracy, and stability, with potential pathways toward higher-order extensions and applications to other convection-diffusion systems.
Abstract
In the finite volume framework, a Lax-Wendrof type second-order flux solver for the compressible Navier-Stokes equations is proposed by utilizing a hyperbolic relaxation model. The flux solver is developed by applying the generalized Riemann problem (GRP) method to the relaxation model that approximates the compressible Navier-Stokes equations. The GRP-based flux solver includes the effects of source terms in numerical fluxes and treats the stiff source terms implicitly, allowing a CFL condition conventionally used for the Euler equations. The trade-off is to solve linear systems of algebraic equations. The resulting numerical scheme achieves second-order accuracy within a single stage, and the linear systems are solved only once in a time step. The parameters to establish the relaxation model are allowed to be locally determined at each cell interface, improving the adaptability to diverse flow regions. Numerical tests with a wide range of flow problems, from nearly incompressible to supersonic flows with strong shocks, for both inviscid and viscous problems, demonstrate the high resolution of the current second-order scheme.
