带有上游圆柱串列布置的海豹须后流激振动与尾流动力学

S. Dulac, Seyedmohammad Mousavisani, T. Breault, B. Seyed-Aghazadeh
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引用次数: 0

摘要

实验研究了与上游圆柱串列布置的柔性密封须模组在横流方向上的流致振动。在U* = 3.2 ~ 24.2的降速范围内,即雷诺数Re = 279 ~ 2077的雷诺数范围内,研究了晶须模块的FIV振荡振幅和振荡频率。研究了上游圆柱体与晶须模块之间较大范围的分离距离,以及晶须面对迎面而来的气流的角度(迎角),并对流致振动响应进行了表征。使用体积粒子跟踪测速法(PTV)数据,通过“Shake the Box”(STB)算法进行处理,可以对须状物模块尾迹中的流场进行时间分辨、三维(3D)三分量(3C)测量,测量须状物模型后的瞬时体积流场。在不同迎角条件下,研究了晶须模块与上游圆柱串联对的尾迹动力学。我们的研究结果表明,当晶须模块以0°迎角放置时,它不会经历任何流动引起的振动。然而,当上游圆柱体与晶须模块串联放置时,晶须在很宽的流速范围内经历了大幅度的振荡。晶须模块收集了留在上游圆柱体后面的“足迹”,中心到中心的距离可达晶须直径的25倍。当上游圆柱体放置在50倍晶须直径的较大距离时,未观察到振荡。当晶须以90°迎角放置时,无论是独立配置的晶须,还是与上游圆柱体串联布置的晶须,都可以在很宽但有限的减速范围内观察到大幅度的振荡。这种在有限流速范围内的大幅度振荡,而振荡频率保持在系统固有频率附近,类似于在弹性安装的圆柱体中观察到的经典涡激振动响应。体积流场测量揭示了在晶须模块的尾迹中高度三维的旋涡脱落模式,这归因于晶须的波动展向结构。当上游圆柱体与下游晶须模块之间的间隙较小时,间隙区域的尾迹表现为存在两个剪切层,并重新附着在下游晶须模块上。随着间隙尺寸的增大,在间隙区域可以观察到发育良好的、高度三维的涡状结构。
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Flow-Induced Vibration and Wake Flow Dynamics Behind a Harbor Seal Whisker Model in Tandem Arrangement With an Upstream Cylinder
Flow-induced vibrations (FIV) of a flexibly-mounted harbor seal whisker module, allowed to oscillate in the cross-flow direction, placed in tandem arrangement with an upstream circular cylinder is studied, experimentally. The FIV response of the whisker module in terms of amplitudes and frequencies of oscillation are studied for a reduced velocity range of U* = 3.2–24.2, corresponding to a Reynolds number range of Re = 279–2,077. Flow-induced vibration response is studied and characterized for a wide range of separation distances between the upstream cylinder and the whisker module, as well as the angle at which the whisker faces the oncoming flow (angle of attack). Instantaneous volumetric flow field behind the whisker model was measured using Volumetric Particle Tracking Velocimetry (PTV) data processed by the “Shake The Box” (STB) algorithm that allowed for the time resolved, three dimensional (3D) 3 components (3C) measurement of flow field in the wake of the whisker module. The wake dynamics of the tandem pair of the whisker module and the upstream cylinder were studied at different angles of attack of the whisker module. Our results show while the whisker module was placed at 0° angle of attack, it did not experience any flow-induced vibration. However, when an upstream cylinder was placed in tandem with the whisker module, the whisker experienced large amplitude oscillations over a wide range of flow velocities. The whisker module picked up the “footprints” left behind the upstream cylinder for center-to center distance up to 25 times the whisker’s diameter. No oscillation was observed when the upstream cylinder was placed at relatively large distance of 50 times the whisker diameter. When the whisker was placed at 90° angle of attack, both for the standalone configuration of the whisker, as well as the tandem arrangement with the upstream cylinder, large amplitude oscillation were observed over a wide, but limited range of reduced velocities. This type of large-amplitude oscillation over a limited range of the flow velocity, while the frequency of oscillation stayed around the natural frequency of the system resembled those classic vortex-induced vibration response observed in the case of an elastically-mounted circular cylinder. Volumetric flow field measurements revealed highly three-dimensional vortex shedding patterns in the wake of the whisker module, which were attributed to the undulatory spanwise structure of the whisker. When the gap size between the upstream cylinder and the downstream whisker module was small, the wake in the gap region was characterized by the presence of two shear layers that were reattached to downstream whisker module. As the gap size increased, well-developed, highly three-dimensional vortical structures were observed in the gap region.
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