A third-order subcell finite volume gas-kinetic scheme for the Euler and Navier-Stokes equations on triangular meshes

被引:6
作者
Zhang, Chao [1 ]
Li, Qibing [1 ]
机构
[1] Tsinghua Univ, Dept Engn Mech, AML, Beijing 100084, Peoples R China
基金
中国国家自然科学基金;
关键词
Gas-kinetic scheme; Subcell finite volume method; High-order methods; Triangular meshes; DISCONTINUOUS GALERKIN METHOD; ESSENTIALLY NONOSCILLATORY SCHEMES; CONSERVATION-LAWS; UNSTRUCTURED GRIDS; II EXTENSION; BGK SCHEME; FLOW; RECONSTRUCTION; EFFICIENT; SOLVER;
D O I
10.1016/j.jcp.2021.110245
中图分类号
TP39 [计算机的应用];
学科分类号
081203 ; 0835 ;
摘要
A third-order gas-kinetic scheme (GKS) based on the subcell finite volume (SCFV) method is developed for the Euler and Navier-Stokes equations on triangular meshes, in which a computational cell is subdivided into four subcells. The scheme combines the compact high-order reconstruction of the SCFV method with the high-order flux evolution of the gas-kinetic solver. Different from the original SCFV method using weighted least square reconstruction along with a conservation correction, a constrained least-square reconstruction is adopted in SCFV-GKS so that the correction is not necessary and continuous polynomials inside each main cell can be reconstructed. For flows with large gradients, a compact hierarchical WENO limiting is adopted. In the gas-kinetic flux solver, the inviscid and viscous flux are coupled and computed simultaneously. Moreover, the spatial and temporal evolution are coupled nonlinearly which enables the developed scheme to achieve third-order accuracy in both space and time within a single stage. As a result, no quadrature point is required for the flux evaluation and the multi-stage Runge-Kutta method is unnecessary as well. A third-order k-exact finite volume GKS is also constructed with the help of k-exact reconstruction. Compared to the k-exact GKS, SCFV-GKS is compact, and with less computational cost for the reconstruction which is based on the main cell. Besides, a continuous reconstruction can be adopted in SCFV-GKS among subcells in smooth flow regions, which results in less numerical dissipation and less computational cost for flux evolution. Thus the efficiency of SCFV-GKS is much higher. Numerical tests demonstrate the strong robustness, high accuracy and efficiency of SCFVGKS in a wide range of flow problems from nearly incompressible to supersonic flows with strong shock waves. (C) 2021 Elsevier Inc. All rights reserved.
引用
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页数:24
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