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Turbulent wake behind side-by-side flat plates: computational study of interference effects

机译:并排平板后面的湍流唤醒:对干扰效应的计算研究

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The complex wake behind two side-by-side flat plates placed normal to the inflow direction has been explored in a direct numerical simulation study. Two gaps, g = 0.5d and 1.0d, were considered, both at a Reynolds number of 1000 based on the plate width d and the inflow velocity. For gap ratio g/d = 0.5, the biased gap flow resulted in an asymmetric flow configuration consisting of a narrow wake with strong vortex shedding and a wide wake with no periodic near-wake shedding. Shear-layer transition vortices were observed in the wide wake, with characteristic frequency 0.6. For g/d = 1.0, two simulations were performed, started from a symmetric and an asymmetric initial flow field. A symmetric configuration of Karman vortices resulted from the first simulation. Surprisingly, however, two different three-dimensional instability features were observed simultaneously along the span of the upper and lower plates. The spanwise wavelengths of these secondary streamwise vortices, formed in the braid regions of the primary Karman vortices, were approximately 1d and 2d, respectively. The wake bursts into turbulence some 5d-10d downstream. The second simulation resulted in an asymmetric wake configuration similar to the asymmetric wake found for the narrow gap 0.5d, with the appearance of shear-layer instabilities in the wide wake. The analogy between a plane mixing layer and the separated shear layer in the wide wake was examined. The shear-layer frequencies obtained were in close agreement with the frequency of the most amplified wave based on linear stability analysis of a plane mixing layer.
机译:在直接数值模拟研究中探讨了垂直于流入方向的两个并排平板后面的复杂唤醒。考虑两个间隙,G = 0.5d和1.0d,基于板宽度d和流入速度,返回雷诺数为1000。对于间隙比率G / D = 0.5,偏置间隙流动导致不对称的流量配置,该流动构造包括具有强大的涡旋脱落的狭窄唤醒,并且没有周期性的近醒来脱落。在宽尾部观察到剪切层过渡涡旋,特征频率为0.6。对于G / D = 1.0,执行了两种模拟,从对称和非对称初始流场开始。由第一模拟产生的Karman扭转物的对称配置。然而,令人惊讶的是,沿着上板和下板的跨度同时观察到了两个不同的三维不稳定性特征。在主Karman涡流的编织区域中形成的这些次级流动涡旋的始线波长分别为约1D和2D。醒来的卷曲变为湍流下游约5d-10d。第二模拟导致不对称的唤醒配置类似于窄间隙0.5d的不对称唤醒,在宽唤醒中具有剪切层稳定性的外观。检查宽尾脉冲层和分离的剪切层之间的类比。获得的剪切层频率与基于平面混合层的线性稳定性分析的基于线性稳定性分析密切一致。

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