Coalescence Behaviors of Drop Swarms on Liquid-Liquid Interface

The trajectory model of dispersed phase drops and distribution model of drop diameters were derived. By numerical simulation, the analytical results indicate that a large number of dispersed phase drops accumulate on the upper plate in different directions and form a hydrodynamic area with the strea...

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Published in:Transactions of Tianjin University Vol. 17; no. 2; pp. 96 - 102
Main Author: 唐洪涛 陈建平 崔世海
Format: Journal Article
Language:English
Published: Heidelberg Tianjin University 01-04-2011
School of Mechanical Engineering, Tianjin University, Tianjin 300072, China
School of Mechanical Engineering, Tianjin University of Science and Technology, Tianjin 300222, China%School of Mechanical Engineering, Tianjin University of Science and Technology, Tianjin 300222, China
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Abstract The trajectory model of dispersed phase drops and distribution model of drop diameters were derived. By numerical simulation, the analytical results indicate that a large number of dispersed phase drops accumulate on the upper plate in different directions and form a hydrodynamic area with the stream-wise location in the range of 0-0.4 m, where the flow of trickling film obtains kinetic drive from flowing field. The flowing field of trickling film exhibits an unstable state if the stream-wise location is less than 0.02 m, and a stable state otherwise. Moreover, different velocity vectors of drops in the x-y plane result in different interactions between the trickling film and drops. For the non-uniform distribution of drop diameters, there is a stronger interaction between the trickling film and drop if the stream-wise location is less than 0.02 m, because the amplitudes of velocity vectors are higher than those in the range of 0.02-1.0 m. The result reveals a complexity and diversity of stratified two-phase flowing field. On the other hand, both the basic flowing field and distributions of drop diameters have a great influence on the distributions of compara- ble kinetic energy of drops. The complicated motions of larger drops are helpful to coalescence because they will con- sume much more kinetic energy on the trickling film than those of smaller drops. The change of comparable kinetic energy of smaller drops is continuous and steady. The smaller drops are easily entrained by the liquid-liquid flowing field.
AbstractList The trajectory model of dispersed phase drops and distribution model of drop diameters were derived. By numerical simulation, the analytical results indicate that a large number of dispersed phase drops accumulate on the upper plate in different directions and form a hydrodynamic area with the stream-wise location in the range of 0–0.4 m, where the flow of trickling film obtains kinetic drive from flowing field. The flowing field of trickling film exhibits an unstable state if the stream-wise location is less than 0.02 m, and a stable state otherwise. Moreover, different velocity vectors of drops in the x-y plane result in different interactions between the trickling film and drops. For the non-uniform distribution of drop diameters, there is a stronger interaction between the trickling film and drop if the stream-wise location is less than 0.02 m, because the amplitudes of velocity vectors are higher than those in the range of 0.02–1.0 m. The result reveals a complexity and diversity of stratified two-phase flowing field. On the other hand, both the basic flowing field and distributions of drop diameters have a great influence on the distributions of comparable kinetic energy of drops. The complicated motions of larger drops are helpful to coalescence because they will consume much more kinetic energy on the trickling film than those of smaller drops. The change of comparable kinetic energy of smaller drops is continuous and steady. The smaller drops are easily entrained by the liquid-liquid flowing field.
O357.4; The trajectory model of dispersed phase drops and distribution model of drop diameters were derived. By numerical simulation, the analytical results indicate that a large number of dispersed phase drops accumulate on the upper plate in different directions and form a hydrodynamic area with the stream-wise location in the range of 0-0.4 m, where the flow of trickling film obtains kinetic drive from flowing field. The flowing field of trickling film exhibits an unstable state if the stream-wise location is less than 0.02 m, and a stable state otherwise. Moreover, different velocity vectors of drops in the x-y plane result in different interactions between the trickling film and drops. For the non-uniform distribution of drop diameters, there is a stronger interaction between the trickling film and drop if the stream-wise location is less than 0.02 m, because the amplitudes of velocity vectors are higher than those in the range of 0.02-1.0 m. The result reveals a complexity and diversity of stratified two-phase flowing field. On the other hand,both the basic flowing field and distributions of drop diameters have a great influence on the distributions of comparable kinetic energy of drops. The complicated motions of larger drops are helpful to coalescence because they will consume much more kinetic energy on the trickling film than those of smaller drops. The change of comparable kinetic energy of smaller drops is continuous and steady. The smaller drops are easily entrained by the liquid-liquid flowing field.
The trajectory model of dispersed phase drops and distribution model of drop diameters were derived. By numerical simulation, the analytical results indicate that a large number of dispersed phase drops accumulate on the upper plate in different directions and form a hydrodynamic area with the stream-wise location in the range of 0-0.4 m, where the flow of trickling film obtains kinetic drive from flowing field. The flowing field of trickling film exhibits an unstable state if the stream-wise location is less than 0.02 m, and a stable state otherwise. Moreover, different velocity vectors of drops in the x-y plane result in different interactions between the trickling film and drops. For the non-uniform distribution of drop diameters, there is a stronger interaction between the trickling film and drop if the stream-wise location is less than 0.02 m, because the amplitudes of velocity vectors are higher than those in the range of 0.02-1.0 m. The result reveals a complexity and diversity of stratified two-phase flowing field. On the other hand, both the basic flowing field and distributions of drop diameters have a great influence on the distributions of compara- ble kinetic energy of drops. The complicated motions of larger drops are helpful to coalescence because they will con- sume much more kinetic energy on the trickling film than those of smaller drops. The change of comparable kinetic energy of smaller drops is continuous and steady. The smaller drops are easily entrained by the liquid-liquid flowing field.
Author 唐洪涛 陈建平 崔世海
AuthorAffiliation School of Mechanical Engineering, Tianjin University, Tianjin 300072, China School of Mechanical Engineering, Tianjin University of Science and Technology, Tianjin 300222, China
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Cites_doi 10.1002/ceat.270140103
10.1016/0009-2509(93)80292-X
10.1016/S0301-9322(99)00109-3
10.1007/s12209-010-1465-4
10.1016/0095-8522(63)90008-4
10.1016/0009-2509(67)80047-2
10.1016/0009-2509(92)80006-X
10.1002/ceat.270100134
10.1016/0009-2509(68)89047-5
10.1002/aic.10075
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Issue 2
Keywords drop
coalescence
diameter
distribution
trajectory
Language English
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Notes drop
TQ464.4
coalescence
O572.243
diameter
12-1248/T
trajectory; coalescence; drop; diameter; distribution
distribution
trajectory
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Snippet The trajectory model of dispersed phase drops and distribution model of drop diameters were derived. By numerical simulation, the analytical results indicate...
O357.4; The trajectory model of dispersed phase drops and distribution model of drop diameters were derived. By numerical simulation, the analytical results...
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SubjectTerms Engineering
Humanities and Social Sciences
Mechanical Engineering
multidisciplinary
Science
分布模型
强相互作用
水滴尺寸
液液界面
稳定状态
速度矢量
Title Coalescence Behaviors of Drop Swarms on Liquid-Liquid Interface
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