论文标题
在粘性流体中两个圆柱体旋转引起的流动
Flow induced by the rotation of two circular cylinders in a viscous fluid
论文作者
论文摘要
通过分析技术和数值技术研究了两个平行圆柱体旋转的旋转驱动的低旋转螺丝流动。在第一部分中,考虑了反旋转缸的情况。通过将系统封闭在半径$ r_ {0} \!\ gg \!1 $的外部圆柱中,获得了数值(有限元)解决方案,并在其上施加了无滑动条件。首先要准确求解具有相同对称性的模型问题,并确定Stokes近似的有效性极限。该模型与睫状推进有一定的意义。对于两缸问题,注意力集中在小空白情况上$ \ varepsilon \ ll 1 $。在接触限制$ \ varepsilon = 0 $中获得了精确的分析解决方案,并且确定了在此接触限制中作用在此圆柱上的净力$ f_ {c} $的净力;这有助于每个圆柱体对其轴的扭矩。还确定了远场扭矩双线(“ Torquelet”)。 第二部分对待共旋转缸的情况,为$ r_ {0} \!\ gg \!1 $获得了有限元数值解决方案。沃森(Watson,1995)的理论被阐明并证明与数值解决方案非常吻合。与反旋转案例相反,在整个流体域中,惯性效应都可以忽略不计,但是提供了$ \ ll 1 $。 在总结部分中,汇总了两种情况的主要结果,并且讨论了液体不受限制的情况($ r_ {0} = \ infty $)。 (...)
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. (...)