4.5 Article

Turbulence simulations with an improved interior penalty discontinuous Galerkin method and SST k-ω model

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COMPUTERS & FLUIDS
卷 263, 期 -, 页码 -

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PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.compfluid.2023.105967

关键词

Discontinuous Galerkin method; RANS simulation; interior penalty method; Computational Fluid Dynamics

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The feasibility of the high-precision interior penalty discontinuous Galerkin (IPDG) method is examined when using the SST k-ω model and its compressibility correction. Turbulence simulations have been conducted using the improved IPDG method and SST k-ω model. The accuracy and reliability of the improved IPDG method, as well as the effectiveness of the compressibility correction, have been validated through numerical simulations and comparison with experimental data.
The feasibility of high-precision interior penalty discontinuous Galerkin (IPDG) method is still questionable when SST k-& omega; model and its compressibility correction are adopted. To this end, turbulence simulations with an improved IPDG method and SST k-& omega; model have been conducted in the present study. In detail, the improved IPDG method was first introduced to eliminate the fourth-order homogeneity tensor connecting the viscous terms and variable gradients. The numerical accuracy has been systematically validated with several canonical cases. To overcome the numerical instability problem coming along with turbulence model simulation, a hybrid approach was implemented. Actually, finite volume method was utilized here for SST k-& omega; model. Then, the accuracy and reliability of the improved IPDG method have been analyzed in accompany with SST k-& omega; model and its compressibility correction. Actually, simulations of subsonic, transonic and supersonic cases have been conducted, including plate/airfoil boundary layers and shear layers. The accuracy has been comprehensively validated through quantitative comparison with experimental data, while the superiority of the compressibility correction could be observed at high Mach number.

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