Numerical simulation of single bubble rising in vertical and inclined square channel using lattice Boltzmann method

被引:27
作者
Amaya-Bower, Luz [2 ]
Lee, Taehun [1 ]
机构
[1] CUNY City Coll, Dept Mech Engn, New York, NY 10031 USA
[2] CUNY, Dept Mech Engn Technol, New York City Coll Technol, Brooklyn, NY 11201 USA
基金
美国国家科学基金会;
关键词
Bubble; Fluid mechanics; Inclined channel; Lattice Boltzmann method; Multiphase flow; Numerical analysis; LONG BUBBLES; SEMIINFINITE BUBBLE; VISCOUS-FLUID; TRAIN FLOW; MOTION; CAPILLARIES; DEPOSITION; DRIVEN; WALL;
D O I
10.1016/j.ces.2010.11.043
中图分类号
TQ [化学工业];
学科分类号
0817 ;
摘要
A lattice Boltzmann equation (LBE) model based on the Cahn-Hilliard diffuse interface approach is used to investigate the dynamics of a bubble rising in a vertical and inclined square channel with large density and viscosity ratios. Deformation parameter Delta, film thickness delta, and terminal velocity U-t of the bubble are interrelated quantities which depend on non-dimensional numbers such as Bond number Bo, Morton number Mo, and ratio between bubble diameter and channel width k as it was reported by previous experimental studies. As k is increased, higher D and smaller d are exhibited. This finding is independent of the value of Bo and Mo. In addition, a relationship was established between delta and Delta with non-dimensional numbers such as Capillary number Ca and Weber number We. An evaluation was performed for inclined channels to relate the Froude number Fr with the inclination angle theta, where in each case there is a critical value of theta which corresponds to the highest value of Fr, consequently highest U-t. This finding is consistent with previous simulation and experimental results. Moreover, a relation was established between the critical value of theta and Ca and Bo. This three-dimensional study was performed using a range of Bo (1 < Bo < 12), Mo (10(-4) < Mo < 10(3)) and the inclination of the channel is varied from 0 to 75 degrees. (C) 2010 Elsevier Ltd. All rights reserved.
引用
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页码:935 / 952
页数:18
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