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Vortex-induced vibration of elastically-mounted spheres: A comparison of the response of three degrees of freedom and one degree of freedom systems

机译:涡旋诱导的弹性安装球体的振动:三种自由度和一种自由度系统的响应进行比较

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In published literature of the vortex-induced vibration of a sphere, limited attention has been devoted to spheres having three degrees of freedom (DOF) motion and the effect on the vibration response. In this study, the vortex-induced vibration response of a 3-DOF elastically-mounted sphere was examined numerically. The response of a sphere allowed to oscillate in all three spatial directions (3-DOF motion) was compared with the response of a sphere whose motion was restricted to only the transverse direction (1-DOF). Simulations were conducted over the reduced velocity range U* U/(Df(n)) is an element of [3.5, 16], using a sphere of mass ratio m* rho(s)/rho = 3, at a fixed Reynolds number of 2000, where U is the free-stream velocity of the flow, f(n) is the natural frequency of the system, rho(s) and rho are the solid and fluid densities, respectively. When the sphere was allowed 3-DOF movement, it was initially excited to vibrate along a linear path in the transverse direction, synchronized with the two-sided shedding of vortex loops behind the sphere. As the simulation time advanced, the sphere trajectory eventually converted into a circular orbit with a spiralling wake behind it. The transition time between these two modes was found to increase with decreasing Reynolds number. The vibration amplitude was significantly smaller when the sphere motion was in all three spatial directions than when it was restricted only to the transverse direction. The maximum vibration amplitudes were approximately 0.6 and 0.8 diameters, for 3-DOF and 1-DOF motion, respectively. In the synchronization regime, the maximum time-averaged drag coefficient was approximately 100% greater than that of a stationary sphere, when the sphere had 3-DOF, similar to previous observations for a tethered sphere. However, the maximum change to the time-averaged drag coefficient was only 76% when the motion was restricted to the transverse direction. (C) 2019 Elsevier Ltd. All rights reserved.
机译:在出版的涡旋诱导的球体振动的文献中,有限的注意力已经致力于具有三个自由度(DOF)运动的球体和对振动响应的影响。在该研究中,在数值上检查了弹性安装的球体的3-DOF的涡旋诱导的振动响应。将允许在所有三个空间方向上振荡的球体(3-DOF运动)的响应与运动被限制为横向(1-DOF)的响应进行比较。在减小的速度范围内进行模拟,U * U /(DF(n))是[3.5,16]的元素,其使用质量比m * rho(s)/ rho = 3的范围,在固定的reynolds号在2000中,你是流量的自由流速度,F(n)是系统的自然频率,rho(s)和rho分别是固体和流体密度。当球体被允许3-DOF运动时,首先激发沿横向的线性路径振动,与球体后面的涡旋环的双面脱落同步。随着仿真时间先进,球体轨迹最终转换成圆形轨道,螺旋形锯齿呈螺旋形式。发现这两种模式之间的过渡时间随着雷诺数的降低而增加。当球体运动处于所有三个空间方向时,振动幅度明显较小,而不是仅在横向上限制时。对于3-DOF和1-DOF运动,最大振动幅度约为0.6和0.8直径。在同步状态下,当球体具有3-DOF时,最大时间平均阻力系数大约超过固定球的拖动系数大约100%。然而,当运动被限制在横向时,时间平均阻力系数的最大变化仅为76%。 (c)2019年elestvier有限公司保留所有权利。

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