Surface tension effects on the behaviour of a rising bubble driven by buoyancy force
In the inviscid and incompressible fluid flow regime,surface tension effects on the behaviour of an initially spherical buoyancy-driven bubble rising in an infinite and initially stationary liquid are investigated numerically by a volume of fluid (VOF) method. The ratio of the gas density to the liq...
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Published in | Chinese physics B Vol. 19; no. 2; pp. 392 - 400 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
IOP Publishing
01.02.2010
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Subjects | |
Online Access | Get full text |
ISSN | 1674-1056 2058-3834 |
DOI | 10.1088/1674-1056/19/2/026801 |
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Abstract | In the inviscid and incompressible fluid flow regime,surface tension effects on the behaviour of an initially spherical buoyancy-driven bubble rising in an infinite and initially stationary liquid are investigated numerically by a volume of fluid (VOF) method. The ratio of the gas density to the liquid density is 0.001, which is close to the case of an air bubble rising in water. It is found by numerical experiment that there exist four critical Weber numbers We1,~We2,~We3 and We4, which distinguish five different kinds of bubble behaviours. It is also found that when 1≤We2, the bubble will finally reach a steady shape, and in this case after it rises acceleratedly for a moment, it will rise with an almost constant speed, and the lower the Weber number is, the higher the speed is. When We 〉We2, the bubble will not reach a steady shape, and in this case it will not rise with a constant speed. The mechanism of the above phenomena has been analysed theoretically and numerically. |
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AbstractList | In the inviscid and incompressible fluid flow regime,surface tension effects on the behaviour of an initially spherical buoyancy-driven bubble rising in an infinite and initially stationary liquid are investigated numerically by a volume of fluid (VOF) method. The ratio of the gas density to the liquid density is 0.001, which is close to the case of an air bubble rising in water. It is found by numerical experiment that there exist four critical Weber numbers We1,~We2,~We3 and We4, which distinguish five different kinds of bubble behaviours. It is also found that when 1≤We2, the bubble will finally reach a steady shape, and in this case after it rises acceleratedly for a moment, it will rise with an almost constant speed, and the lower the Weber number is, the higher the speed is. When We 〉We2, the bubble will not reach a steady shape, and in this case it will not rise with a constant speed. The mechanism of the above phenomena has been analysed theoretically and numerically. In the inviscid and incompressible fluid flow regime, surface tension effects on the behaviour of an initially spherical buoyancy-driven bubble rising in an infinite and initially stationary liquid are investigated numerically by a volume of fluid (VOF) method. The ratio of the gas density to the liquid density is 0.001, which is close to the case of an air bubble rising in water. It is found by numerical experiment that there exist four critical Weber numbers We1, We2, We3 and We4, which distinguish five different kinds of bubble behaviours. It is also found that when 1 <= We < We2, the bubble will finally reach a steady shape, and in this case after it rises acceleratedly for a moment, it will rise with an almost constant speed, and the lower the Weber number is, the higher the speed is. When We > We2, the bubble will not reach a steady shape, and in this case it will not rise with a constant speed. The mechanism of the above phenomena has been analysed theoretically and numerically. |
Author | 王含 张振宇 杨永明 张慧生 |
AuthorAffiliation | Department of Mechanics and Engineering Science, Fudan University, Shanghai 200433, China Department of Mathematics, Shanghai University of Finance and Economics, Shanghai 200433, China |
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Cites_doi | 10.1017/S0022112063001373 10.1088/1674-1056/17/10/051 10.1016/j.jcp.2006.06.020 10.1063/1.861445 10.1017/S002211208100311X 10.1006/jcph.1998.5906 10.1017/S0022112059000520 10.1016/S0021-9991(03)00087-1 10.1098/rspa.1950.0023 10.1016/0021-9991(92)90307-K 10.1017/S0022112099004449 10.1017/S0022112062000300 10.1006/jcph.2000.6658 10.1103/PhysRevE.71.066302 10.1016/j.jcp.2006.08.008 10.1017/S0022112097005570 10.1103/PhysRevE.70.056310 10.1017/S0022112084002226 10.1017/S0022112064000349 10.1016/0021-9991(81)90145-5 |
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References | 11 22 23 13 Wan D C (18) 1998; 15 14 15 Wang H (20) 2008; 17 17 19 Liu R X (12) 2003 Zou J F (16) 2002; 16 1 2 Batchelor G K (24) 1967 3 4 5 6 7 8 9 10 21 |
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Snippet | In the inviscid and incompressible fluid flow regime,surface tension effects on the behaviour of an initially spherical buoyancy-driven bubble rising in an... In the inviscid and incompressible fluid flow regime, surface tension effects on the behaviour of an initially spherical buoyancy-driven bubble rising in an... |
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SubjectTerms | Bubbles Buoyancy Density Incompressible flow Liquids Mathematical models Surface tension Weber number 上升气泡 不可压缩 数值实验 气泡行为 流体流动 浮力驱动 表面张力 高速度 |
Title | Surface tension effects on the behaviour of a rising bubble driven by buoyancy force |
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