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首页> 外文期刊>Journal of Fluid Mechanics >Dynamics of an inverted cantilever plate at moderate angle of attack
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Dynamics of an inverted cantilever plate at moderate angle of attack

机译:倒悬臂板处于适度攻角的动态

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The dynamics of a cantilever plate clamped at its trailing edge and placed at a moderate angle (alpha <= 30 degrees) to a uniform flow are investigated experimentally and numerically, and a large experimental data set is provided. The dynamics are shown to differ significantly from the zero-angle-of-attack case, commonly called the inverted-flag configuration. Four distinct dynamical regimes arise at non-zero angles: a small oscillation around a small-deflection equilibrium (deformed regime), a small-amplitude flapping motion, a large-amplitude flapping motion and a small oscillation around a large-deflection equilibrium (deflected regime). The small- and large-amplitude flapping motions are shown to be produced by different physical mechanisms. The small-amplitude flapping motion appears gradually as the flow speed is increased and is consistent with a limit-cycle oscillation caused by the quasi-steady fluid forcing. The large-amplitude flapping motion is observed to appear at a constant critical flow speed that is independent of angle of attack. Its characteristics match those of the large-amplitude vortex-induced vibration present at zero angle of attack. The flow speed at which the plate enters the deflected regime decreases linearly as the angle of attack is increased, causing the flapping motion to disappear for angles of attack greater than alpha approximate to 28 degrees. Finally, the effect of aspect ratio on the plate dynamics is considered, with a plate of reduced aspect ratio being shown to lack a sharp distinction between flapping regimes for alpha > 8 degrees.
机译:本文对夹持在后缘并与均匀流成中等角度(α≤30°)的悬臂板的动力学进行了实验和数值研究,并提供了大量实验数据集。动态显示与零攻角情况(通常称为倒旗配置)有显著差异。在非零角度下出现四种不同的动力学状态:围绕小挠度平衡的小振动(变形状态)、小振幅扑动、大振幅扑动和围绕大挠度平衡的小振动(偏转状态)。小振幅和大振幅的拍打运动被证明是由不同的物理机制产生的。随着流速的增加,小振幅扑翼运动逐渐出现,这与准稳态流体强迫引起的极限环振荡一致。观察到大振幅的扑翼运动出现在与攻角无关的恒定临界流速下。其特性与零攻角下的大振幅涡激振动相匹配。当迎角增大时,板块进入偏转区域的流动速度线性降低,导致当迎角大于alpha(约28度)时,拍打运动消失。最后,考虑了长宽比对板动力学的影响,结果表明,长宽比减小的板在α>8度的拍动区域之间缺乏明显的区别。

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