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Control of flow past a circular cylinder via a spanwise surface wire: effect of the wire scale

机译:通过展向表面导线控制流过圆柱的流量:导线刻度的影响

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Flow phenomena induced by a single spanwise wire on the surface of a circular cylinder are investigated via a cinema technique of particle image velocimetry (PIV). The primary aim of this investigation is to assess the effect of the wire scale. To this end, consideration is given to wires with different diameters that are 0.5, 1.2, and 2.9% of the cylinder diameter. The Reynolds number has a subcritical value of 10,000. Compared to the thickness of the unperturbed boundary layer developing around the cylinder between 5° and 75° from the forward stagnation point, the former two wires have smaller scales and the latter has a larger scale. Two angular locations of the wire, defined with respect to the forward stagnation point of the cylinder, are found to be critical. When the wire is located at these critical angles, either the most significant extension or the contraction of the time-mean separation bubble occurs in the near wake. These critical angles depend on the wire scale: the smaller the wire, the larger the critical angle. The small-scale and large-scale wires that have diameters of 1.2 and 2.9% of the cylinder diameter induce bistable shear-layer oscillations between different separation modes when placed at their respective critical angles corresponding to maximum extension of the near-wake bubble. These oscillations have irregular time intervals that are much longer than the time scale associated with the classical Kármán instability. Moreover, the large-scale wire can either significantly attenuate or intensify the Kármán mode of vortex shedding at the critical states; in contrast, the small-scale wires do not notably alter the strength of the Kármán instability.
机译:通过电影图像测速技术(PIV)研究了由单根翼展方向的金属丝在圆柱体表面上引起的流动现象。这项研究的主要目的是评估线规的影响。为此,要考虑直径分别为圆柱直径的0.5%,1.2%和2.9%的电线。雷诺数的次临界值为10,000。与从前停滞点开始在5°到75°之间在圆柱体周围形成的不受扰动边界层的厚度相比,前两条线的比例较小,而后者的比例较大。发现相对于圆柱体的向前停滞点定义的线的两个角位置是关键的。当导线处于这些临界角时,时间均值分离气泡的最明显的延伸或收缩会在近尾时发生。这些临界角取决于导线比例:导线越小,临界角越大。当直径分别为圆柱直径的1.2%和2.9%的小尺寸和大尺寸导线以对应于接近尾迹气泡最大扩展的临界角放置时,会在不同的分离模式之间引起双稳态剪切层振荡。这些振荡具有不规则的时间间隔,该时间间隔比与经典的卡尔曼不稳定性相关的时间尺度长得多。而且,大型导线可以显着衰减或增强临界状态下涡旋脱落的Kármán模式。相比之下,小尺寸电线不会明显改变Kármán不稳定性的强度。

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