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Numerical study of shock-wave/turbulent boundary layer interactions on flexible panels with wall-modeled large-eddy simulations

机译:具有壁图的大涡模拟柔性面板冲击/湍流边界层相互作用的数值研究

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Coupled fluid structure interaction (FSI) simulations with wall-modeled LES (WMLES) are used to capture the interaction of an oblique shock impinging on the turbulent boundary layer developed along a flexible panel. The simulations replicate prior experiments conducted at the trisonic wind tunnel (TMK) of the Supersonic and Hypersonic Technologies Department at DLR, Cologne. The flow has a freestream Math number M_∞ = 3.0, and an incoming turbulent boundary layer thickness δ_0 = 4 mm upstream of the interaction. It is impinged by an oblique shock generated by a rotating wedge with a maximum deflection angle θ_(max) = 17.5°, reached approximately 15 ms after starting from a zero wedge angle corresponding to a shock-free panel. Displacement signals over time at different panel locations are compared to the experiments and to a previous FSI numerical wall-resolved large-eddy simulation. The effect of flexibility on the wall pressure as a function of streamwise location and time is assessed, showing a modulation by the panel vibration that affects the full panel streamwise extent. Wall pressure power spectral densities show an elongation of the frequency band associated with flow separation region for the flexible case over the nominal rigid configuration. Additionally, the turbulent boundary layer of the flexible panel takes a longer distance to recover downstream of the oblique shock. The peak contribution of the low frequency motions to the power spectrum is increased for the flexible case. The study of separation bubble dynamics reveals that panel flexibility increases the separation length and volume, but leaves the bubble streamwise centroid nearly unaffected.
机译:耦合流体结构相互作用(FSI)模拟具有壁图的LES(WMLE),用于捕获冲击沿着柔性面板开发的湍流边界层的倾斜冲击的相互作用。模拟在DLR,科隆DLR的超音速和超声波技术部门的三色风洞(TMK)进行了先前的实验。该流程具有FreeSteam Math NumberM_‖= 3.0,并且在交互上游Δ_0= 4mm的进入的湍流边界层厚度Δ_0= 4mm。它通过旋转楔形产生的倾斜冲击,最大偏转角θ_(max)= 17.5°,从对应于无减震面板的零楔角开始之后达到大约15ms。将不同面板位置的位移信号随时间与实验进行比较,并以先前的FSI数值壁分辨的大涡模拟。评估作为流动位置和时间的函数的柔性对壁压力的影响,显示了面板振动的调制,影响全面板的流动范围。壁压力功率谱密度显示与柔性壳体上的流动分离区域相关联的频带伸长率,用于在标称刚性配置上。另外,柔性面板的湍流边界层需要更长的距离以恢复倾斜冲击的下游。对于柔性壳体,增加了低频运动对功率谱的峰值贡献。分离气泡动力学的研究表明,面板柔韧性增加了分离长度和体积,但留下了泡沫流的质心,几乎不受影响。

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