Simple bladeless mixer with liquid–gas interface

IF 2.8 Q2 MECHANICS
Daiki Watanabe, S. Goto
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引用次数: 2

Abstract

Abstract A constantly rotating spherical container sustains turbulence of a fluid partially filling it. This simple turbulence generator has the potential for wide engineering applications as a bladeless mixer. Using the coupled level-set and volume of fluid method and the boundary data immersion method, we conduct direct numerical simulations of liquid–gas flow in a spherical container rotating about a horizontal axis to investigate the driving mechanism of turbulence, flow dependence on the filling rate $\varPsi$ and the mixing ability of the sustained turbulence. Even if the Froude number $Fr$ is small enough ($Fr\lesssim 10^{-3}$) for the liquid–gas interface to be undeformed, if the Reynolds number $Re$ is large enough ($Re\gtrsim 10^3$), small-scale turbulent eddies are sustained by being stretched in shear flow around a counter-rotating pair of container-size vortices, whose swirling directions depend on $\varPsi$. We clarify that the angle of flow near the solid wall colliding with the interface controls the swirling direction of these container-size vortices. Furthermore, we track fluid particles in the liquid phase to quantify mixing properties to show that almost perfect mixing occurs after approximately 10 spins of the container for lower $\varPsi$ ($\lesssim 0.5$), whereas the mixing requires less energy consumption for higher $\varPsi$ ($\gtrsim 0.7$) at the examined $Re=O(10^3)$.
具有液气界面的简单无叶片混合器
一个不断旋转的球形容器承受着部分填充其中的流体的湍流。这种简单的湍流发生器作为无叶片混合器具有广泛的工程应用潜力。采用水平集与流体体积耦合法和边界数据浸没法,对沿水平轴旋转的球形容器内液气流动进行了直接数值模拟,探讨了湍流的驱动机制、对填充率的依赖以及持续湍流的混合能力。即使弗鲁德数$Fr$足够小($Fr\lesssim 10^{-3}$)使液气界面保持不变,如果雷诺数$Re$足够大($Re\gtrsim 10^3$),小规模的湍流漩涡通过在剪切流中围绕一对反向旋转的容器大小的漩涡而被拉紧,其旋转方向取决于$\varPsi$。研究表明,固体壁面附近与界面碰撞的气流角度控制着这些容器大小的涡流的旋转方向。此外,我们跟踪液相中的流体颗粒以量化混合特性,结果表明,在较低$\varPsi$ ($\lesssim 0.5$)条件下,容器在大约10次旋转后发生了几乎完美的混合,而在所检查的$Re=O(10^3)$条件下,较高$\varPsi$ ($\gtrsim 0.7$)条件下,混合需要较少的能量消耗。
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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来源期刊
CiteScore
2.40
自引率
0.00%
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0
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