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Numerical investigations of shock wave interactions with a supersonic turbulent boundary layer

机译:超音速湍流边界层与激波相互作用的数值研究

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摘要

Direct numerical simulations (DNS) are conducted for a Mach 2.75 turbulent boundary layer interacting with an impinging shock at three different shock incidence angles. The accuracies of DNS calculations are established by checking the convergence of flow statistics for various grids, by comparing the generated results with those in the literature and also by the balance of contributing terms in the turbulent kinetic energy equation. Instantaneous flow visualizations show the significant effect of shock on turbulence structure in the shock-boundary layer interaction zone and also in the flow downstream of the interaction region. The separation bubbles exhibit highly unsteady and three-dimensional behavior and are larger for stronger shocks but the maximum probability of flow separation is found to be independent of the shock strength. The differences between Reynolds- and Favre-averaged quantities are also observed to be small and largely independent of the shock intensity. The turbulent kinetic energy is amplified across the shock, mainly by the production term in the turbulent kinetic energy equation. The amplification of enstrophy across the shock zone is found to be due to the vortex stretching term in the enstrophy transport equation. A detailed examination of the terms in the turbulent kinetic equation shows a strong coupling between the mean and turbulent fields in the interaction region with energy being continuously exchanged from one field to another. However, the compressibility-related terms in the transport equations for turbulent kinetic energy and enstrophy are found to be small for the simulated flows.
机译:对马赫数为2.75的湍流边界层在三个不同的冲击入射角与冲击冲击相互作用进行了直接数值模拟(DNS)。通过检查各种网格的流量统计数据的收敛性,比较生成的结果与文献中的结果以及湍流动能方程中各贡献项之间的平衡,可以确定DNS计算的准确性。瞬时流动可视化显示了冲击对冲击边界层相互作用区域以及相互作用区域下游流动中湍流结构的显着影响。分离气泡表现出高度的不稳定和三维行为,并且对于较强的冲击较大,但发现流动分离的最大概率与冲击强度无关。雷诺数和法弗平均数之间的差异也很小,并且很大程度上与冲击强度无关。湍动能在整个冲击过程中被放大,主要是通过湍动能方程中的乘积项。发现整个激波区的涡旋放大是由于涡旋传输方程中的涡旋拉伸项引起的。对湍流动力学方程中各项的详细研究表明,相互作用区域中的平均场和湍流场之间存在强耦合,能量从一个场连续交换到另一个场。但是,对于模拟流动,湍流动能和涡流的输运方程中与可压缩性有关的项很小。

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