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Numerical Simulation of Vortex-Induced Vibration with Three-Step Finite Element Method and Arbitrary Lagrangian-Eulerian Formulation

机译:三步有限元法和任意拉格朗日-欧拉公式的涡激振动数值模拟

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Numerical simulations were performed in this paper to investigate an elastically mounted circular cylinder subjected to vortex-induced vibration (VIV). A three-step finite element method (FEM) is introduced for solving the incompressible fluid flow equations in two dimensions. The computational procedure is coupled with a mesh movement scheme by use of the arbitrary Lagrangian-Eulerian (ALE) formulation on account of the body motion in the flow field. On running the numerical simulations, the Reynolds number was kept constant of Re = 100 and the reduced velocity U_r = U/(f_nD) was varied from 3.0 to 10.2 by changing the natural frequency f_n of the cylinder. The mass ratio m* = 4m/ρπD~2 and damping ratio ξ are set to be 10.0 and 0.01, respectively, where U is free-stream velocity, D the diameter of the circular cylinder, m the mass of the cylinder per unit length, and ρ the density of the fluid. Numerical results are examined for the response amplitude of transverse direction as well as the phase angle, φ, between the lift force and the transverse displacement of the cylinder. The numerical results reveal that the transverse amplitudes present only two branches, namely, initial branch and lower branch, rather than three branches as the results obtained from high-Re experiments with low m~*ξ. On the other hand, the phase angles present almost linear increase with the reduced velocity in the synchronization region. However, experiments concerned with high Re exhibit a sudden jump in phase angle of approximate 180°. The difference between the present study and the high-Re experiment is attributed to no substantial vortex shedding mode transition at the present numerical results of laminar flow.
机译:在本文中进行了数值模拟,以研究受到涡旋振动(VIV)的弹性安装圆柱体。引入了三步有限元方法(FEM)来求解二维不可压缩流体流动方程。考虑到流场中的身体运动,通过使用任意拉格朗日-欧拉(ALE)公式,将计算过程与网格运动方案相结合。在运行数值模拟时,雷诺数保持Re = 100不变,并且通过更改圆柱的固有频率f_n,降低的速度U_r = U /(f_nD)从3.0变为10.2。质量比m * = 4m /ρπD〜2和阻尼比ξ分别设置为10.0和0.01,其中U是自由流速度,D是圆柱直径,m是每单位长度的圆柱质量,ρ为流体的密度。检验了数值结果的横向响应幅度以及气缸升力和横向位移之间的相位角φ。数值结果表明,横向振幅仅存在两个分支,即初始分支和较低分支,而不是由低m〜*ξ的高Re实验获得的三个分支。另一方面,随着同步区域中速度的降低,相位角几乎呈线性增加。但是,与高Re有关的实验显示出相角大约为180°的突然跳跃。本研究与高分辨率实验之间的差异归因于目前层流数值结果中没有实质的涡旋脱落模式转变。

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