arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2008.04432physics.flu-dyn

粘性流体中两个圆筒旋转引起的流动

Flow induced by the rotation of two circular cylinders in a viscous fluid

E. Dormy, H. K. Moffatt

AI总结:

本文用解析和数值方法研究粘性流体中两平行圆筒旋转产生的低雷诺数流动,分别分析反向和同向旋转,确定力与扭矩并验证理论,揭示惯性效应差异。

摘要:

本文通过解析和数值技术研究了两个等半径单位平行圆筒在低雷诺数下的斯托克斯流动。第一部分考虑反向旋转圆筒的情况。通过将系统封闭在半径为$R_{0}\gg 1$的外圆筒内并施加无滑移条件,获得了数值(有限元)解。首先精确求解了一个具有相同对称性的模型问题,并确定了斯托克斯近似的有效极限;该模型对纤毛推进具有一定意义。对于双圆筒问题,重点关注小间隙情况$\varepsilon \ll 1$。在接触极限$\varepsilon=0$下获得了精确解析解,并确定了在该接触极限下作用于圆筒对的净力$F_{c}$;该力对每个圆筒绕其轴所承受的扭矩有贡献。还识别了远场扭矩偶极子(“扭矩子”)。第二部分处理同向旋转圆筒的情况,同样在$R_{0}\gg 1$下获得了有限元数值解。阐明了Watson(1995)的理论,并显示其与数值解吻合良好。与反向旋转情况相反,在整个流体域中,无论多大,只要Re $\ll 1$,惯性效应均可忽略。在结论部分,总结了两种情况的主要结果,并讨论了流体无界($R_{0}=\infty$)的情况。

英文摘要:

The low-Reynolds-number Stokes flow driven by rotation of two parallel cylinders of equal unit radius is investigated by both analytical and numerical techniques. In Part I, the case of counter-rotating cylinders is considered. A numerical (finite-element) solution is obtained by enclosing the system in an outer cylinder of radius $R_{0}\!\gg\!1$, on which the no-slip condition is imposed. A model problem with the same symmetries is first solved exactly, and the limit of validity of the Stokes approximation is determined; this model has some relevance for ciliary propulsion. For the two-cylinder problem, attention is focused on the small-gap situation $\varepsilon \ll 1$. An exact analytic solution is obtained in the contact limit $\varepsilon=0$, and a net force $F_{c}$ acting on the pair of cylinders in this contact limit is identified; this contributes to the torque that each cylinder experiences about its axis. The far-field torque doublet (`torquelet') is also identified. Part II treats the case of co-rotating cylinders, for which again a finite-element numerical solution is obtained for $R_{0}\!\gg \!1$. The theory of Watson (1995) is elucidated and shown to agree well with the numerical solution. In contrast to the counter-rotating case, inertia effects are negligible throughout the fluid domain, however large, provided Re $\ll 1$. In the concluding section, the main results for both cases are summarised, and the situation when the fluid is unbounded ($R_{0}=\infty$) is discussed. (...)

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