Investigation of vortex packet recovery in perturbed turbulent boundary layers

Y. Tan, E. Longmire
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Abstract

Turbulent boundary layers (Reτ = 2500) were perturbed by a spanwise array of cylinders with spacing of S= 0.2δ, where δ is the unperturbed boundary layer thickness. Two cylinder heights were considered, H = 0.2δ (H = 500) and H = δ. Although visualizations suggest that disrupted packet signatures downstream of the H = δ array re-organized from bottom up, autocorrelation magnitudes along the streamwise direction for the flow at z = 125 were reduced relative to unperturbed values up to 7δ downstream of the array suggesting that flow features unrelated to packets remained altered there. On the other hand, spectral energy in large spanwise scales recovered substantially at the same location. For the H = 0.2δ case, previous results showed disrupted packet signatures re-appearing beginning 2δ downstream at z = 300, while packet signatures at z = 500 persisted through the array, supporting a top-down reorganization. However, spanwise characteristics of flow features closer to the wall (z = 125) remained altered relative to the unperturbed flow up to 7δ downstream yet streamwise length scales from autocorrelations at z = 125 and x = 7δ matched unperturbed values. Interestingly, the shape of the spanwise energy spectrum at this location resembled shapes of spectra in planes above, suggesting outer-layer influence.
扰动湍流边界层中涡包恢复的研究
湍流边界层(Reτ = 2500)被间距为S= 0.2δ的横向圆柱阵列扰动,其中δ为未扰动边界层厚度。考虑两种圆柱高度,H = 0.2δ (H = 500)和H = δ。虽然可视化显示,H = δ阵列下游的中断数据包特征从下向上重新组织,但z = 125处流动沿流向的自相关强度相对于阵列下游高达7δ的未扰动值有所减少,这表明与数据包无关的流特征在那里仍然发生了变化。另一方面,在大跨度尺度上,光谱能量在同一位置得到了大幅度的恢复。对于H = 0.2δ的情况,先前的结果表明,中断的数据包签名从z = 300开始在下游2δ处重新出现,而z = 500处的数据包签名在数组中持续存在,支持自上而下的重组。然而,靠近壁面(z = 125)的流动特征的展向特征相对于未扰动的下游7δ流动仍然发生变化,但z = 125和x = 7δ的自相关的流向长度尺度与未扰动的值相匹配。有趣的是,这个位置的能谱与上面平面上的能谱形状相似,表明受到了外层的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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