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Large-eddy simulation of multi-component compressible turbulent flows using high resolution methods

机译:利用高分辨率方法对多组分可压缩湍流进行大涡模拟

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The ability of a finite volume Godunov and a semi-Lagrangian large-eddy simulation (LES) method to predict shock induced turbulent mixing has been examined through simulations of the half-height experiment [Holder and Barton. In: Proceedings of the international workshop on the physics of compressible turbulent mixing, 2004]. Very good agreement is gained in qualitative comparisons with experimental results for combined Richtmyer-Meshkov and Kelvin-Helmholtz instabilities in compressible turbulent multi-component flows. It is shown that both numerical methods can capture the size, location and temporal growth of the main flow features. In comparing the methods, there is variability in the amount of resolved turbulent kinetic energy. The semi-Lagrangian method has constant dissipation at low Mach number, thus allowing the initially small perturbations to develop into Kelvin-Helmholtz instabilities. These are suppressed at the low Mach stage in the Godunov method. However, there is an excellent agreement in the final amount of fluid mixing when comparing both numerical methods at different grid resolutions.
机译:有限体积的Godunov和半拉格朗日大涡模拟(LES)方法预测冲击引起的湍流混合的能力已通过半高实验的模拟进行了检验[Holder和Barton。在:可压缩湍流混合物理学国际研讨会论文集,2004年]。定性比较与可压缩湍流多组分流中Richtmyer-Meshkov和Kelvin-Helmholtz联合不稳定性的实验结果获得了很好的一致性。结果表明,两种数值方法都可以捕获主流特征的大小,位置和时间增长。在比较这些方法时,解析出的湍动能的数量存在差异。半拉格朗日方法在低马赫数下具有恒定的耗散,因此允许最初的小扰动发展为开尔文-亥姆霍兹不稳定性。这些在Godunov方法的低马赫阶段被抑制。但是,在不同网格分辨率下比较两种数值方法时,流体混合的最终量存在着极好的共识。

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