Streaming Fluid Motion Within a Laterally Oscillating Sphere With Density Stratification.

IF 0.8
D Kong, S Zhang, A Penkova, A Y Rednikov, S S Sadhal
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Abstract

In this investigation, we have examined the fundamental problem of streaming motion in a liquid-filled sphere undergoing lateral oscillations. Such motion can be externally created, or exists in spacecrafts where [Formula: see text]-jitter is well known. The important point here is that for spatially constant liquid density, such an internal problem is degenerate, when no non-trivial oscillatory flow and hence no streaming occur. However, this totally changes in the presence of some density stratification, which may be due to compositional and/or thermal non-uniformities. To clarify the phenomenon in simplest possible terms, we here just consider a constant volumetric heating source within the liquid and isothermal container walls. Proceeding with oscillatory displacement of the spherical shell, we assume a high-frequency limit relative to the viscous and thermal times, and a small displacement amplitude relative to the container (sphere) size. Treating the oscillations as a perturbation to an otherwise stationary shell, two steady streaming contributions are revealed. One is driven in the bulk of the liquid, which is atypical in the incompressible-liquid limit. The other classically originates in the Stokes layer at the boundary also engaging the bulk by viscosity. Even if the former is asymptotically greater here, it does not turn out to be practical to outright disregard the latter. The reason is the particularly low prefactor values arising in the former, which is typical for the internal problem. The streaming pattern consists of two or four axially symmetric vortices, which are dependent on the result of the competition between the two contributions.

具有密度分层的横向振荡球体内的流动流体运动。
在这项研究中,我们研究了在一个充满液体的球体中进行横向振荡的流运动的基本问题。这种运动可以由外部产生,也可以存在于众所周知的抖动的航天器中。这里重要的一点是,对于空间恒定的液体密度,这样的内部问题是简并的,当没有非平凡的振荡流动,因此没有流动发生。然而,在存在一些密度分层时,这种情况完全改变,这可能是由于成分和/或热不均匀性造成的。为了用最简单的术语解释这一现象,我们在这里只考虑液体和等温容器壁上的定容热源。继续处理球壳的振荡位移,我们假设相对于粘性和热时间有一个高频极限,相对于容器(球体)尺寸有一个小的位移振幅。将振荡视为对静止壳的扰动,揭示了两个稳定流的贡献。一个是在大量液体中驱动的,这在不可压缩液体极限中是非典型的。另一种通常起源于边界处的斯托克斯层,也通过黏性与体体接触。即使前者在这里逐渐增大,完全忽视后者也不现实。原因是前者产生的前因子值特别低,这是典型的内部问题。流型由两个或四个轴对称涡旋组成,取决于两个涡旋之间的竞争结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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