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LES of shock wave/turbulent boundary layer interaction affected by microramp vortex generators

机译:受微斜坡涡发生器影响的冲击波/湍流边界层相互作用的LES

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摘要

At large Mach numbers, the interaction of an oblique shock wave with a turbulent boundary layer (SWTBLI) developing over a flat plate gives rise to a separation bubble known to exhibit low-frequency streamwise oscillations around StL = 0.03 (a Strouhal number based on the separated region length). Because these oscillations yield wall pressure or load fluctuations, efforts are made to reduce their amplitude. We perform large eddy simulations to reproduce the experiments by Wang etal (2012) where a rake of microramp vortex generators (MVGs) were inserted upstream the SWTBLI with consequences yet to be fully understood. There is no consensus on the flow structure downstream MVGs and this is first clarified in the case of MVGs protruding by 0.47δ in a TBL at Mach number M = 2.7 and Reynolds number Reθ = 3600. Large-scale vortices intermittently shed downstream the MVGs are characterized by a streamwise period close to twice the TBL thickness and a frequency f ≈ 0.5Ue/δ, two orders of magnitude higher than the one of the uncontrolled SWTBLI. We then characterize the interaction between the unsteady wake of the MVGs with the SWTBLI resulting in the reduction of the interaction length and the high-frequency modulation of the shock feet motions.
机译:在大马赫数下,倾斜冲击波与平板上形成的湍流边界层(SWTBLI)的相互作用产生了一个分离气泡,该分离气泡在StL = 0.03周围表现出低频的流向振荡(基于分隔区域的长度)。由于这些振荡会产生壁压或负载波动,因此需要努力降低其幅度。我们执行大型涡流模拟以重现Wang等人(2012)的实验,其中在SWTBLI的上游插入了微斜坡涡发生器(MVG)的耙子,其后果尚待充分理解。对于下游MVG的流动结构尚无共识,这首先在MVG在马赫数M = 2.7和雷诺数Reθ= 3600的TBL中以0.47δ突出的情况下得到澄清。间歇性地掉落在MVG下游的大型旋涡是其特点是沿流向的周期接近TBL厚度的两倍,频率f≈0.5Ue /δ,比不受控制的SWTBLI之一高两个数量级。然后,我们表征了MVG与SWTBLI的非稳定唤醒之间的相互作用,从而导致了相互作用长度的减小和电击脚运动的高频调制。

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