圆圆柱体和方圆柱体振荡流动的数值研究

A. Okajima, T. Yasuda
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摘要

本文采用数值模拟方法研究了静止流体中振荡钝体周围的流型和作用在钝体上的力。本文采用ALE(任意拉格朗日-欧拉)有限差分法模拟了淹没在静水中的振荡钝体(如圆柱体和方形体)的流动。在二维和三维、非定常、不可压缩和粘性流动的假设下进行了模拟。数值模拟的预测结果与我们最近的测量结果进行了比较,该结果设置在u型管水箱产生的平面振荡流中,在Keulegan Carpenter (KC)数为30和β值为95和153时,对钝体的流动力和流动的可视化模式进行了测量。虽然钝体周围的流型是由钝体涡脱落和平面振荡流共同产生的复杂流型,但实验中观察到的主要涡脱落型、低KC数下的“三维结构”流型、“横街”流型和“双对”流型都可以在本模拟中成功地再现,并且模拟流型与实测流型之间有很好的一致性。对于具有不同形状截面的钝体(如圆形截面和方形截面)周围的流动配置,也证实了显著的差异。预测和测量的直线力之间也有很好的一致性,即阻力和惯性系数CD, CM的值,由著名的莫里森方程表示,以及波动横向力(升力)CL在KC值范围内。此外,值得注意的是,依赖于KC数的横向力值与流型变化的过程很好地对应。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Numerical Study of Oscillatory Flow Around Circular and Square Cylinders
The flow patterns around and the forces acting on an oscillating bluff body submerged in a fluid at rest have been studied by numerical simulations. An ALE (Arbitrary Lagrangian-Eulerian) finite difference method has been employed to simulate the flow around an oscillating bluff body, e.g., a circular cylinder and a square one, submerged in a still water. Simulations have been carried out under the assumption of 2- and 3-dimensional, unsteady, incompressible and viscous flow. The results predicted by numerical simulations are compared with our recent results of measurements of fluiddynamic forces on and flow-visualized patterns around a bluff body that is set in a planar oscillatory flow generated by a U-tube water tank up to Keulegan Carpenter (KC) numbers of 30 and at a value of β of 95 and 153. Although flow-patterns around a bluff body are complicatedly produced by both the vortex-shedding from a bluff body and the planar oscillatory flow, the major vortex-shedding regimes observed in experiments, flow pattern of “3-dimensional structures” at low KC numbers, “transverse street” and “double pair” all can be successfully reproduced in the present simulations, and there is good agreement between the simulated and measured flow patterns. Notable differences are also confirmed for flow configurations around a bluff body with a different shaped-section, e.g., a circular section and a square one. There is found to be good agreement also between the predicted and measured in-line forces, i.e., the values of drag and inertia coefficients, CD, CM, represented by the well-known Morison’s equation and the fluctuating transverse force (lift force) CL across a range of KC values. Furthermore, it is noteworthy that the values of transverse force depending on KC numbers correspond well to the process of flow pattern variation.
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