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Wake-boundary layer interaction behind an elliptic cylinder at different Reynolds numbers

机译:不同雷诺数椭圆缸背后的唤醒边界层相互作用

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In this paper, hot-wire anemometry (HWA) is used to experimentally investigate interactions between a fully developed turbulent boundary layer and wake of an elliptic cylinder where axis ratio (AR) of the cylinder is 2. The elliptic cylinder was located inside and outside a turbulent boundary layer with a thickness () of 0.38B. Furthermore, experiments were conducted at different Reynolds numbers (13,250 and 26,500) based upon the smallest cylinder diameter (B). Mean velocity, turbulence intensity and higher-order central moments of velocity signals (i.e. skewness and flatness) measurements were performed using HWA upon wake-boundary layer interactions on a flat plate. Results showed that profiles of stream-wise mean velocity and turbulence intensity were greatly dependent on gap ratio (G/B) and Reynolds number (Re) in near-wake region. It was also observed that, except for G/B= 0.1, the wake-boundary layer interactions were faster at Reynolds number of 26,500 rather than 13,250. The interactions occurred earlier upon fluctuating the velocity rather than the case where a fixed mean velocity was considered. The results further show that an increase in the gap ratio increases Strouhal number almost independent of /B. Behind the cylinder, relatively smaller wake region was obtained at Re= 26,500 rather than Re= 13,250, where the velocity profiles quickly converged to the flat plate boundary layer velocity profiles.
机译:在本文中,热线风化术(HWA)用于通过实验研究完全发育的湍流边界层与椭圆圆筒的唤醒之间的相互作用,其中汽缸的轴线比(AR)为2.椭圆圆柱位于内部和外部湍流边界层,厚度为0.38b。此外,基于最小的汽缸直径(B),在不同的雷诺数(13,250和26,500)处进行实验。在平板上的唤醒边界层相互作用时,使用HWA对速度信号(即偏斜和平坦度)测量的平均速度,湍流强度和高阶中心测量。结果表明,近苏醒区域的流动式平均速度和湍流强度的曲线大大依赖于间隙比(G / B)和雷诺数(RE)。还观察到,除了G / B = 0.1之外,雷诺数为26,500而不是13,250的雷诺数的唤醒层相互作用。在波动速度而不是考虑固定平均速度的情况下,更早地发生相互作用。结果进一步表明,间隙比的增加几乎独立于/ b。在汽缸后面,在Re = 26,500处而不是Re = 13,250,在速度速度迅速地聚合到平板边界层速度轮廓上的相对较小的唤醒区域。

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