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Boundary-element simulation of hydrodynamic interaction of two smooth spheres suspended in an unbounded Couette flow

机译:悬浮在无界库埃特流中的两个光滑球体的水动力相互作用的边界元模拟

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The hydrodynamic interaction between two particles, suspended in shear flows, is fundamental to the macroscopic characterization of suspension flows. Although the understanding of the hydrodynamic interaction between two particles suspended in a quiescent or linear shear flow is mature, studies of the interaction in a non-linear shear field are rare. The current study calculates such interactions between two neutrally-buoyant smooth spheres moving at negligible Reynolds numbers in an unbounded wide-gap Couette flow by three-dimensional boundary-element method (BEM) simulations. Both the identical sphere-pair and the disparate sphere-pair are considered. The numerical results show that there is a preferential cross-streamline migration of the center-of-gravity of the sphere-pair in the plane of shear in the unbounded wide-gap Couette flow that does not arise in simple shear-flow. This migration is always directed towards low-shear regions when the sphere having the larger translational velocity approaches the other sphere, and reverses towards high-shear regions when the faster sphere leads the other sphere in the plane of shear. There is also a cross-streamline migration of the center-of-gravity of the sphere-pair in the plane of vorticity, but this migration does not have a preferential direction. These migrations are symmetric about the point where the spheres are at the minimum separation, and are only significant when the hydrodynamic interaction of the spheres is sufficiently strong. These results show that the migration of the center- of-gravity of the sphere-pair can be attributed to the non-linearity of the shear field. The hydrody-namic interaction between the two spheres has been quantified under various conditions by the BEM simulations for both identical and disparate spheres.
机译:悬浮在剪切流中的两个颗粒之间的水动力相互作用是悬浮流的宏观表征的基础。尽管对悬浮在静态或线性剪切流中的两个粒子之间的流体动力相互作用的理解已经成熟,但是在非线性剪切场中相互作用的研究却很少。当前的研究通过三维边界元方法(BEM)模拟计算了在无界宽间隙库埃特流中以可忽略的雷诺数运动的两个中性浮力光滑球体之间的相互作用。相同的球对和不同的球对都被考虑。数值结果表明,在无边界宽间隙库埃特流中,球对的重心在剪切平面中存在优先的跨流线迁移,这在简单剪切流中不会发生。当具有较大平移速度的球接近另一个球体时,该迁移总是指向低剪切区域,而当较快的球体在剪切平面中领先于另一个球体时,这种迁移总是指向高剪切区域。球对的重心在涡旋平面中也有跨流线的迁移,但是这种迁移没有优先方向。这些迁移是关于球体处于最小间距的点对称的,并且仅当球体的流体动力相互作用足够强时才有意义。这些结果表明,球对重心的迁移可以归因于剪切场的非线性。已经通过BEM模拟在相同和不同球体的各种条件下对两个球体之间的水动力相互作用进行了定量。

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