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arXiv 2007.14172physics.flu-dynphysics.bio-ph
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二维格点拍动平板的集体运动

Collective locomotion of two-dimensional lattices of flapping plates

Silas Alben

摘要:

本文研究了不可压流场中矩形和菱形格点拍动板在雷诺数为O(10- 100)时的推进特性。我们改变五个参数:拍打幅度、频率(或雷诺数)、板之间的水平和垂直间距以及迎面而来的流体流速度。在流向方向上紧密排列的格子在相邻的板之间产生强烈的涡流偶极子。当这些偶极子在临界流速下从上游方向切换到下游方向时,晶格从产生阻力急剧过渡到产生推力。在这些转变附近,流动呈现出各种周期性和非周期性状态,有或没有上下对称性,并且可以出现多个稳定的自推进速度。随着流向间距的增加,板可能会脱落撞击下游相邻板的典型涡流尾流。由于横向间距小,矩形网格产生净阻力,而菱形网格可能产生净推力,有时效率很高。随着横向间距的增加,矩形网格开始产生推力,最终效率略高于菱形网格,因为这两种类型的网格流会聚。在Re = 70时,时间周期格子流的最大弗劳德效率约为孤立板的两倍。在较低的Re下,网格的效率优势增加,直到孤立的扑动板不再产生推力。在小间隙和大流向间距的限制下,分别在两种情况下,板之间的小间隙和Poiffille-like流动,可以估计产生格子流所需的平均输入功率。对于这两种晶格,随着横向间距变大(并发生推力),平均输入功率饱和。在小的横向间距下,当板重叠时,菱形晶格的输入功率可能大得多,导致弗劳德效率降低。

英文摘要:

We study the propulsive properties of rectangular and rhombic lattices of flapping plates at O(10--100) Reynolds numbers in incompressible flow. We vary five parameters: flapping amplitude, frequency (or Reynolds number), horizontal and vertical spacings between plates, and oncoming fluid stream velocity. Lattices that are closely spaced in the streamwise direction produce intense vortex dipoles between adjacent plates. The lattices transition sharply from drag- to thrust-producing as these dipoles switch from upstream to downstream orientations at critical flow speeds. Near these transitions the flows assume a variety of periodic and nonperiodic states, with and without up-down symmetry, and multiple stable self-propelled speeds can occur. As the streamwise spacing increases, the plates may shed typical vortex wakes that impinge on downstream neighbors. With small lateral spacing, rectangular lattices yield net drag, while rhombic lattices may generate net thrust, sometimes with high efficiency. As lateral spacing increases, rectangular lattices begin to generate thrust, eventually with slightly higher efficiencies than rhombic lattices, as the two types of lattice flows converge. At Re = 70, the maximum Froude efficiencies of time-periodic lattice flows are about twice those of an isolated plate. At lower Re, the lattices' efficiency advantage increases until the isolated flapping plate no longer generates thrust. The mean input power needed to generate the lattice flows can be estimated in the limits of small and large streamwise spacings, with small-gap and Poiseuille-like flows between the plates respectively in the two cases. For both lattices, the mean input power saturates as the lateral spacing becomes large (and thrust occurs). At small lateral spacings, the rhombic lattices' input power may be much larger when the plates overlap, leading to a decrease in Froude efficiency.

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