Mukundakrishnan Karthik, Quan Shaoping, Eckmann David M, Ayyaswamy Portonovo S
Department of Anesthesiology and Critical Care, University of Pennsylvania, Philadelphia, Pennsylvania 19104, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2007 Sep;76(3 Pt 2):036308. doi: 10.1103/PhysRevE.76.036308. Epub 2007 Sep 19.
The wall effects on the axisymmetric rise and deformation of an initially spherical gas bubble released from rest in a liquid-filled, finite circular cylinder are numerically investigated. The bulk and gas phases are considered incompressible and immiscible. The bubble motion and deformation are characterized by the Morton number (Mo), Eötvös number (Eo), Reynolds number (Re), Weber number (We), density ratio, viscosity ratio, the ratios of the cylinder height and the cylinder radius to the diameter of the initially spherical bubble ( H*=H/d0, R*=R/d0). Bubble rise in liquids described by Eo and Mo combinations ranging from (1,0.01) to (277.5,0.092), as appropriate to various terminal state Reynolds numbers (ReT) and shapes have been studied. The range of terminal state Reynolds numbers includes 0.02<ReT<70 . Bubble shapes at terminal states vary from spherical to intermediate spherical-cap-skirted. The numerical procedure employs a front tracking finite difference method coupled with a level contour reconstruction of the front. This procedure ensures a smooth distribution of the front points and conserves the bubble volume. For the wide range of Eo and Mo examined, bubble motion in cylinders of height H*=8 and R*> or =3 , is noted to correspond to the rise in an infinite medium, both in terms of Reynolds number and shape at terminal state. In a thin cylindrical vessel (small R*), the motion of the bubble is retarded due to increased total drag and the bubble achieves terminal conditions within a short distance from release. The wake effects on bubble rise are reduced, and elongated bubbles may occur at appropriate conditions. For a fixed volume of the bubble, increasing the cylinder radius may result in the formation of well-defined rear recirculatory wakes that are associated with lateral bulging and skirt formation. The paper includes figures of bubble shape regimes for various values of R*, Eo, Mo, and ReT. Our predictions agree with existing results reported in the literature.
对在充满液体的有限圆柱形容器中从静止释放的初始为球形的气泡的轴对称上升和变形的壁面效应进行了数值研究。液相和气相被视为不可压缩且不互溶的。气泡的运动和变形由莫顿数(Mo)、厄缶数(Eo)、雷诺数(Re)、韦伯数(We)、密度比、粘度比、圆柱高度与圆柱半径相对于初始球形气泡直径的比值(H* = H/d0,R* = R/d0)来表征。研究了由Eo和Mo组合描述的气泡在液体中的上升情况,其范围从(1,0.01)到(277.5,0.092),适用于各种终端状态雷诺数(ReT)和形状。终端状态雷诺数的范围包括0.02 < ReT < 70。终端状态下的气泡形状从球形变化到中间的球冠裙状。数值计算过程采用了前沿跟踪有限差分法,并结合前沿的水平轮廓重建。该过程确保了前沿点的平滑分布并保持了气泡体积。对于所研究的广泛的Eo和Mo范围,高度为H* = 8且R*≥3的圆柱形容器中的气泡运动,在雷诺数和终端状态形状方面都被发现与在无限介质中的上升相对应。在薄壁圆柱形容器(小R*)中,气泡的运动由于总阻力增加而受到阻碍,并且气泡在离释放点很短的距离内就达到了终端条件。尾流对气泡上升的影响减小,并且在适当条件下可能会出现细长的气泡。对于固定体积的气泡,增加圆柱半径可能会导致形成明确的后向再循环尾流,这与横向鼓起和裙边形成有关。本文包括了针对各种R*、Eo、Mo和ReT值的气泡形状区域图。我们的预测与文献中报道的现有结果一致。