Numerical modeling of oscillating Taylor bubbles

In this study, computational fluid dynamics (CFD) modeling is used to simulate Taylor bubbles rising in vertical pipes. Experiments indicate that in large diameter (0.29 m) pipes for an air–water system, the bubbles can rise in a oscillatory manner, depending on the method of air injection. The CFD...

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Main Authors: S. Ambrose, D. M. Hargreaves, I. S. Lowndes
Format: Article
Language:English
Published: Taylor & Francis Group 2016-01-01
Series:Engineering Applications of Computational Fluid Mechanics
Subjects:
Online Access:http://dx.doi.org/10.1080/19942060.2016.1224737
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spelling doaj-6420a60995a6425a9dfccc5289a458812020-11-24T23:56:18ZengTaylor & Francis GroupEngineering Applications of Computational Fluid Mechanics1994-20601997-003X2016-01-0110157859810.1080/19942060.2016.12247371224737Numerical modeling of oscillating Taylor bubblesS. Ambrose0D. M. Hargreaves1I. S. Lowndes2University of NottinghamUniversity of NottinghamUniversity of NottinghamIn this study, computational fluid dynamics (CFD) modeling is used to simulate Taylor bubbles rising in vertical pipes. Experiments indicate that in large diameter (0.29 m) pipes for an air–water system, the bubbles can rise in a oscillatory manner, depending on the method of air injection. The CFD models are able to capture this oscillatory behavior because the air phase is modeled as a compressible ideal gas. Insights into the flow field ahead and behind the bubble during contraction and expansion are shown. For a bubble with an initial pressure equal to the hydrostatic pressure at its nose, no oscillations are seen in the bubble as it rises. If the initial pressure in the bubble is set less than or greater than the hydrostatic pressure then the length of the bubble oscillates with an amplitude that depends on the magnitude of the initial bubble pressure relative to the hydrostatic pressure. The frequency of the oscillations is inversely proportional to the square root of the head of water above the bubble and so the frequency increases as the bubble approaches the water surface. The predicted frequency also depends inversely on the square root of the average bubble length, in agreement with experimental observations and an analytical model that is also presented. In this model, a viscous damping term due to the presence of a Stokes boundary layer for the oscillating cases is introduced for the first time and used to assess the effect on the oscillations of increasing the liquid viscosity by several orders of magnitude.http://dx.doi.org/10.1080/19942060.2016.1224737Numerical simulationTaylor bubblebubble riseoscillationsstokes boundary layer
collection DOAJ
language English
format Article
sources DOAJ
author S. Ambrose
D. M. Hargreaves
I. S. Lowndes
spellingShingle S. Ambrose
D. M. Hargreaves
I. S. Lowndes
Numerical modeling of oscillating Taylor bubbles
Engineering Applications of Computational Fluid Mechanics
Numerical simulation
Taylor bubble
bubble rise
oscillations
stokes boundary layer
author_facet S. Ambrose
D. M. Hargreaves
I. S. Lowndes
author_sort S. Ambrose
title Numerical modeling of oscillating Taylor bubbles
title_short Numerical modeling of oscillating Taylor bubbles
title_full Numerical modeling of oscillating Taylor bubbles
title_fullStr Numerical modeling of oscillating Taylor bubbles
title_full_unstemmed Numerical modeling of oscillating Taylor bubbles
title_sort numerical modeling of oscillating taylor bubbles
publisher Taylor & Francis Group
series Engineering Applications of Computational Fluid Mechanics
issn 1994-2060
1997-003X
publishDate 2016-01-01
description In this study, computational fluid dynamics (CFD) modeling is used to simulate Taylor bubbles rising in vertical pipes. Experiments indicate that in large diameter (0.29 m) pipes for an air–water system, the bubbles can rise in a oscillatory manner, depending on the method of air injection. The CFD models are able to capture this oscillatory behavior because the air phase is modeled as a compressible ideal gas. Insights into the flow field ahead and behind the bubble during contraction and expansion are shown. For a bubble with an initial pressure equal to the hydrostatic pressure at its nose, no oscillations are seen in the bubble as it rises. If the initial pressure in the bubble is set less than or greater than the hydrostatic pressure then the length of the bubble oscillates with an amplitude that depends on the magnitude of the initial bubble pressure relative to the hydrostatic pressure. The frequency of the oscillations is inversely proportional to the square root of the head of water above the bubble and so the frequency increases as the bubble approaches the water surface. The predicted frequency also depends inversely on the square root of the average bubble length, in agreement with experimental observations and an analytical model that is also presented. In this model, a viscous damping term due to the presence of a Stokes boundary layer for the oscillating cases is introduced for the first time and used to assess the effect on the oscillations of increasing the liquid viscosity by several orders of magnitude.
topic Numerical simulation
Taylor bubble
bubble rise
oscillations
stokes boundary layer
url http://dx.doi.org/10.1080/19942060.2016.1224737
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