On the numerical study of bubbly flow created by ventilated cavity in vertical pipe
The dispersion of bubbles into a down-liquid flow in a vertical pipe is investigated. At low flow rates, the intended design of a swarm of discrete bubbles is achieved. At high flow rates, a ventilated cavity is nonetheless formed, which is attached close to the gas sparger. Behind this ventilated c...
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Veröffentlicht in: | International journal of multiphase flow 2011-09, Vol.37 (7), p.756-768 |
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description | The dispersion of bubbles into a down-liquid flow in a vertical pipe is investigated. At low flow rates, the intended design of a swarm of discrete bubbles is achieved. At high flow rates, a ventilated cavity is nonetheless formed, which is attached close to the gas sparger. Behind this ventilated cavity, three different flow regimes characterize the complex bubbly flow field downstream of the down-liquid flow: vortex region with high void fraction, transitional region and pipe flow region. In this study, a numerical model that solved the entire development of the gas–liquid flow including the extended single-phase liquid region upstream to the wall-jet and recirculating-vortex zones in order to allow a more realistic determination of the boundary conditions of the down-liquid flow was adopted. Coupling with the Eulerian–Eulerian two-fluid model to solve the respective gas and liquid phases, a population balance model was also applied to predict the bubble size distribution in the wake right below the cavity base as well as further downstream in the transitional and fully-developed pipe flow regions. The numerical model was evaluated by comparing the numerical results against the data derived from theoretical, numerical and experimental approaches. Prediction of the Sauter mean bubble diameter distributions by the population balance approach at different axial locations confirmed the dominance of breakage due to the high turbulent intensity below the ventilated cavity which led to the generation of small gas bubbles at high void fraction. Further downstream, the coalescence effect dominated leading to merging of the small bubbles to form bigger bubbles. |
doi_str_mv | 10.1016/j.ijmultiphaseflow.2011.01.014 |
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At low flow rates, the intended design of a swarm of discrete bubbles is achieved. At high flow rates, a ventilated cavity is nonetheless formed, which is attached close to the gas sparger. Behind this ventilated cavity, three different flow regimes characterize the complex bubbly flow field downstream of the down-liquid flow: vortex region with high void fraction, transitional region and pipe flow region. In this study, a numerical model that solved the entire development of the gas–liquid flow including the extended single-phase liquid region upstream to the wall-jet and recirculating-vortex zones in order to allow a more realistic determination of the boundary conditions of the down-liquid flow was adopted. Coupling with the Eulerian–Eulerian two-fluid model to solve the respective gas and liquid phases, a population balance model was also applied to predict the bubble size distribution in the wake right below the cavity base as well as further downstream in the transitional and fully-developed pipe flow regions. The numerical model was evaluated by comparing the numerical results against the data derived from theoretical, numerical and experimental approaches. Prediction of the Sauter mean bubble diameter distributions by the population balance approach at different axial locations confirmed the dominance of breakage due to the high turbulent intensity below the ventilated cavity which led to the generation of small gas bubbles at high void fraction. 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At low flow rates, the intended design of a swarm of discrete bubbles is achieved. At high flow rates, a ventilated cavity is nonetheless formed, which is attached close to the gas sparger. Behind this ventilated cavity, three different flow regimes characterize the complex bubbly flow field downstream of the down-liquid flow: vortex region with high void fraction, transitional region and pipe flow region. In this study, a numerical model that solved the entire development of the gas–liquid flow including the extended single-phase liquid region upstream to the wall-jet and recirculating-vortex zones in order to allow a more realistic determination of the boundary conditions of the down-liquid flow was adopted. Coupling with the Eulerian–Eulerian two-fluid model to solve the respective gas and liquid phases, a population balance model was also applied to predict the bubble size distribution in the wake right below the cavity base as well as further downstream in the transitional and fully-developed pipe flow regions. The numerical model was evaluated by comparing the numerical results against the data derived from theoretical, numerical and experimental approaches. Prediction of the Sauter mean bubble diameter distributions by the population balance approach at different axial locations confirmed the dominance of breakage due to the high turbulent intensity below the ventilated cavity which led to the generation of small gas bubbles at high void fraction. Further downstream, the coalescence effect dominated leading to merging of the small bubbles to form bigger bubbles.</description><subject>Bubbles</subject><subject>Bubbly flow</subject><subject>CFD</subject><subject>Computational fluid dynamics</subject><subject>Exact sciences and technology</subject><subject>Flow rate</subject><subject>Flows in ducts, channels, nozzles, and conduits</subject><subject>Fluid dynamics</subject><subject>Fluid flow</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Holes</subject><subject>Mathematical models</subject><subject>Multiphase and particle-laden flows</subject><subject>Nonhomogeneous flows</subject><subject>Physics</subject><subject>Pipe flow</subject><subject>Population balance</subject><subject>Turbulent flow</subject><subject>Ventilated cavity</subject><issn>0301-9322</issn><issn>1879-3533</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNqNUE1LxDAQDaLguvofclFPXWeSfl4EEb9A8KCeQ5pO2SzdtibpSv-9rSsePAkPhhnevMd7jF0grBAwvdqs7GY7NMH2a-2pbrrPlQDEFcyID9gC86yIZCLlIVuABIwKKcQxO_F-AwBJFssFe31peVgTb4ctOWt0w30YqpF3NS-HsmxGPgtz40gHqng58h21wTbfm9E7G0Zu2-nowvd3b3s6ZUe1bjyd_cwle7-_e7t9jJ5fHp5ub54jI4s8RHmKkiojZA4lpIgyrqnIcsoNgQCdZBCTkSmKSteFFkhYYpLpspYlxjmgXLLLvW7vuo-BfFBb6w01jW6pG7zKi1RMHSQz83rPNK7z3lGteme32o0KQc1lqo36W6aay1QwI54Ezn-stJ9i1k63xvpfFRFLSJMUJt7jnkdT7p0lp7yx1BqqrCMTVNXZ_1p-AWZelY0</recordid><startdate>20110901</startdate><enddate>20110901</enddate><creator>Xiang, M.</creator><creator>Cheung, S.C.P.</creator><creator>Yeoh, G.H.</creator><creator>Zhang, W.H.</creator><creator>Tu, J.Y.</creator><general>Elsevier Ltd</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TB</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>KR7</scope><scope>L7M</scope></search><sort><creationdate>20110901</creationdate><title>On the numerical study of bubbly flow created by ventilated cavity in vertical pipe</title><author>Xiang, M. ; Cheung, S.C.P. ; Yeoh, G.H. ; Zhang, W.H. ; Tu, J.Y.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c398t-8613edc2380b061134fe978e8ce020a5704ec3612daf9a21e1b157abf3b148013</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Bubbles</topic><topic>Bubbly flow</topic><topic>CFD</topic><topic>Computational fluid dynamics</topic><topic>Exact sciences and technology</topic><topic>Flow rate</topic><topic>Flows in ducts, channels, nozzles, and conduits</topic><topic>Fluid dynamics</topic><topic>Fluid flow</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Holes</topic><topic>Mathematical models</topic><topic>Multiphase and particle-laden flows</topic><topic>Nonhomogeneous flows</topic><topic>Physics</topic><topic>Pipe flow</topic><topic>Population balance</topic><topic>Turbulent flow</topic><topic>Ventilated cavity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Xiang, M.</creatorcontrib><creatorcontrib>Cheung, S.C.P.</creatorcontrib><creatorcontrib>Yeoh, G.H.</creatorcontrib><creatorcontrib>Zhang, W.H.</creatorcontrib><creatorcontrib>Tu, J.Y.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>International journal of multiphase flow</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Xiang, M.</au><au>Cheung, S.C.P.</au><au>Yeoh, G.H.</au><au>Zhang, W.H.</au><au>Tu, J.Y.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>On the numerical study of bubbly flow created by ventilated cavity in vertical pipe</atitle><jtitle>International journal of multiphase flow</jtitle><date>2011-09-01</date><risdate>2011</risdate><volume>37</volume><issue>7</issue><spage>756</spage><epage>768</epage><pages>756-768</pages><issn>0301-9322</issn><eissn>1879-3533</eissn><coden>IJMFBP</coden><abstract>The dispersion of bubbles into a down-liquid flow in a vertical pipe is investigated. At low flow rates, the intended design of a swarm of discrete bubbles is achieved. At high flow rates, a ventilated cavity is nonetheless formed, which is attached close to the gas sparger. Behind this ventilated cavity, three different flow regimes characterize the complex bubbly flow field downstream of the down-liquid flow: vortex region with high void fraction, transitional region and pipe flow region. In this study, a numerical model that solved the entire development of the gas–liquid flow including the extended single-phase liquid region upstream to the wall-jet and recirculating-vortex zones in order to allow a more realistic determination of the boundary conditions of the down-liquid flow was adopted. Coupling with the Eulerian–Eulerian two-fluid model to solve the respective gas and liquid phases, a population balance model was also applied to predict the bubble size distribution in the wake right below the cavity base as well as further downstream in the transitional and fully-developed pipe flow regions. The numerical model was evaluated by comparing the numerical results against the data derived from theoretical, numerical and experimental approaches. Prediction of the Sauter mean bubble diameter distributions by the population balance approach at different axial locations confirmed the dominance of breakage due to the high turbulent intensity below the ventilated cavity which led to the generation of small gas bubbles at high void fraction. Further downstream, the coalescence effect dominated leading to merging of the small bubbles to form bigger bubbles.</abstract><cop>Kidlington</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.ijmultiphaseflow.2011.01.014</doi><tpages>13</tpages></addata></record> |
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subjects | Bubbles Bubbly flow CFD Computational fluid dynamics Exact sciences and technology Flow rate Flows in ducts, channels, nozzles, and conduits Fluid dynamics Fluid flow Fundamental areas of phenomenology (including applications) Holes Mathematical models Multiphase and particle-laden flows Nonhomogeneous flows Physics Pipe flow Population balance Turbulent flow Ventilated cavity |
title | On the numerical study of bubbly flow created by ventilated cavity in vertical pipe |
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