Phase field lattice Boltzmann model for air-water two phase flows

Two phase flows occur in different forms with liquid and gas in general, among which, the interaction of the flow of air and water is a common scenario. However, modeling the two phase flow still remains a challenge due to the large density ratio between them and different space-time scales involved...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Physics of fluids (1994) 2019-07, Vol.31 (7)
Hauptverfasser: Dinesh Kumar, E., Sannasiraj, S. A., Sundar, V.
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page
container_issue 7
container_start_page
container_title Physics of fluids (1994)
container_volume 31
creator Dinesh Kumar, E.
Sannasiraj, S. A.
Sundar, V.
description Two phase flows occur in different forms with liquid and gas in general, among which, the interaction of the flow of air and water is a common scenario. However, modeling the two phase flow still remains a challenge due to the large density ratio between them and different space-time scales involved in the flow regimes. In the present work, the lattice Boltzmann (LB) model capable of handling large density ratio (1000) and high Reynolds number (104) simultaneously is proposed. The present model consists of two sets of LB equations, one for the flow field in terms of normalized pressure-velocity formulation and the other for the solution of the conservative Allen-Cahn equation to capture the interface. The numerical tests such as stationary drop, bubble coalescence, and capillary wave decay have been performed, and the results exhibit excellent mass conservation property. The capability of the present model to handle complex scenarios has been tested through test cases, for example, rise of an air bubble, splash of a water droplet on a wet bed, and Rayleigh-Taylor instability. In all test cases, the simulation results agree well with the available reference data. Finally, as an application of the present model, the breaking of a deep water wave with high Reynolds number (104) is simulated. The plunging breaker with wave overturning and the generation of secondary jet and splashes are well described by the present LB model. The evolution of wave energy dissipation during and after breaking is in agreement with the reference data.
doi_str_mv 10.1063/1.5100215
format Article
fullrecord <record><control><sourceid>proquest_scita</sourceid><recordid>TN_cdi_proquest_journals_2255928040</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2255928040</sourcerecordid><originalsourceid>FETCH-LOGICAL-c393t-3b8cb8d119f9ba37b0ca8b2f325baf261be261b8c78116ca4df97ee10dabe4193</originalsourceid><addsrcrecordid>eNp90E1LAzEQBuAgCtbqwX8Q8KSwNZN0s8mxFr-goAc9hySb4JbtZk1Si_56W7boQfAyM4dnZuBF6BzIBAhn1zApgRAK5QEaARGyqDjnh7u5IgXnDI7RSUpLQgiTlI_Q7PlNJ4d949oatzrnxjp8E9r8tdJdh1ehdi32IWLdxGKjs4s4bwLuh602bNIpOvK6Te5s38fo9e72Zf5QLJ7uH-ezRWGZZLlgRlgjagDppdGsMsRqYahntDTaUw7G7YqwlQDgVk9rLyvngNTauClINkYXw90-hve1S1ktwzp225eK0rKUVJAp2arLQdkYUorOqz42Kx0_FRC1S0iB2ie0tVeDTbbJOjeh-8EfIf5C1df-P_z38jeTGXO0</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2255928040</pqid></control><display><type>article</type><title>Phase field lattice Boltzmann model for air-water two phase flows</title><source>AIP Journals Complete</source><source>Alma/SFX Local Collection</source><creator>Dinesh Kumar, E. ; Sannasiraj, S. A. ; Sundar, V.</creator><creatorcontrib>Dinesh Kumar, E. ; Sannasiraj, S. A. ; Sundar, V.</creatorcontrib><description>Two phase flows occur in different forms with liquid and gas in general, among which, the interaction of the flow of air and water is a common scenario. However, modeling the two phase flow still remains a challenge due to the large density ratio between them and different space-time scales involved in the flow regimes. In the present work, the lattice Boltzmann (LB) model capable of handling large density ratio (1000) and high Reynolds number (104) simultaneously is proposed. The present model consists of two sets of LB equations, one for the flow field in terms of normalized pressure-velocity formulation and the other for the solution of the conservative Allen-Cahn equation to capture the interface. The numerical tests such as stationary drop, bubble coalescence, and capillary wave decay have been performed, and the results exhibit excellent mass conservation property. The capability of the present model to handle complex scenarios has been tested through test cases, for example, rise of an air bubble, splash of a water droplet on a wet bed, and Rayleigh-Taylor instability. In all test cases, the simulation results agree well with the available reference data. Finally, as an application of the present model, the breaking of a deep water wave with high Reynolds number (104) is simulated. The plunging breaker with wave overturning and the generation of secondary jet and splashes are well described by the present LB model. The evolution of wave energy dissipation during and after breaking is in agreement with the reference data.</description><identifier>ISSN: 1070-6631</identifier><identifier>EISSN: 1089-7666</identifier><identifier>DOI: 10.1063/1.5100215</identifier><identifier>CODEN: PHFLE6</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Aerodynamics ; Air bubbles ; Capillary waves ; Coalescing ; Computational fluid dynamics ; Computer simulation ; Deep water ; Density ratio ; Energy dissipation ; Fluid dynamics ; Fluid flow ; High Reynolds number ; Physics ; Reynolds number ; Taylor instability ; Two phase flow ; Water drops ; Water waves ; Wave power</subject><ispartof>Physics of fluids (1994), 2019-07, Vol.31 (7)</ispartof><rights>Author(s)</rights><rights>2019 Author(s). Published under license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c393t-3b8cb8d119f9ba37b0ca8b2f325baf261be261b8c78116ca4df97ee10dabe4193</citedby><cites>FETCH-LOGICAL-c393t-3b8cb8d119f9ba37b0ca8b2f325baf261be261b8c78116ca4df97ee10dabe4193</cites><orcidid>0000-0002-5788-6696 ; 0000-0003-4440-4771 ; 0000-0001-7421-0543</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,790,4498,27901,27902</link.rule.ids></links><search><creatorcontrib>Dinesh Kumar, E.</creatorcontrib><creatorcontrib>Sannasiraj, S. A.</creatorcontrib><creatorcontrib>Sundar, V.</creatorcontrib><title>Phase field lattice Boltzmann model for air-water two phase flows</title><title>Physics of fluids (1994)</title><description>Two phase flows occur in different forms with liquid and gas in general, among which, the interaction of the flow of air and water is a common scenario. However, modeling the two phase flow still remains a challenge due to the large density ratio between them and different space-time scales involved in the flow regimes. In the present work, the lattice Boltzmann (LB) model capable of handling large density ratio (1000) and high Reynolds number (104) simultaneously is proposed. The present model consists of two sets of LB equations, one for the flow field in terms of normalized pressure-velocity formulation and the other for the solution of the conservative Allen-Cahn equation to capture the interface. The numerical tests such as stationary drop, bubble coalescence, and capillary wave decay have been performed, and the results exhibit excellent mass conservation property. The capability of the present model to handle complex scenarios has been tested through test cases, for example, rise of an air bubble, splash of a water droplet on a wet bed, and Rayleigh-Taylor instability. In all test cases, the simulation results agree well with the available reference data. Finally, as an application of the present model, the breaking of a deep water wave with high Reynolds number (104) is simulated. The plunging breaker with wave overturning and the generation of secondary jet and splashes are well described by the present LB model. The evolution of wave energy dissipation during and after breaking is in agreement with the reference data.</description><subject>Aerodynamics</subject><subject>Air bubbles</subject><subject>Capillary waves</subject><subject>Coalescing</subject><subject>Computational fluid dynamics</subject><subject>Computer simulation</subject><subject>Deep water</subject><subject>Density ratio</subject><subject>Energy dissipation</subject><subject>Fluid dynamics</subject><subject>Fluid flow</subject><subject>High Reynolds number</subject><subject>Physics</subject><subject>Reynolds number</subject><subject>Taylor instability</subject><subject>Two phase flow</subject><subject>Water drops</subject><subject>Water waves</subject><subject>Wave power</subject><issn>1070-6631</issn><issn>1089-7666</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp90E1LAzEQBuAgCtbqwX8Q8KSwNZN0s8mxFr-goAc9hySb4JbtZk1Si_56W7boQfAyM4dnZuBF6BzIBAhn1zApgRAK5QEaARGyqDjnh7u5IgXnDI7RSUpLQgiTlI_Q7PlNJ4d949oatzrnxjp8E9r8tdJdh1ehdi32IWLdxGKjs4s4bwLuh602bNIpOvK6Te5s38fo9e72Zf5QLJ7uH-ezRWGZZLlgRlgjagDppdGsMsRqYahntDTaUw7G7YqwlQDgVk9rLyvngNTauClINkYXw90-hve1S1ktwzp225eK0rKUVJAp2arLQdkYUorOqz42Kx0_FRC1S0iB2ie0tVeDTbbJOjeh-8EfIf5C1df-P_z38jeTGXO0</recordid><startdate>201907</startdate><enddate>201907</enddate><creator>Dinesh Kumar, E.</creator><creator>Sannasiraj, S. A.</creator><creator>Sundar, V.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-5788-6696</orcidid><orcidid>https://orcid.org/0000-0003-4440-4771</orcidid><orcidid>https://orcid.org/0000-0001-7421-0543</orcidid></search><sort><creationdate>201907</creationdate><title>Phase field lattice Boltzmann model for air-water two phase flows</title><author>Dinesh Kumar, E. ; Sannasiraj, S. A. ; Sundar, V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c393t-3b8cb8d119f9ba37b0ca8b2f325baf261be261b8c78116ca4df97ee10dabe4193</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Aerodynamics</topic><topic>Air bubbles</topic><topic>Capillary waves</topic><topic>Coalescing</topic><topic>Computational fluid dynamics</topic><topic>Computer simulation</topic><topic>Deep water</topic><topic>Density ratio</topic><topic>Energy dissipation</topic><topic>Fluid dynamics</topic><topic>Fluid flow</topic><topic>High Reynolds number</topic><topic>Physics</topic><topic>Reynolds number</topic><topic>Taylor instability</topic><topic>Two phase flow</topic><topic>Water drops</topic><topic>Water waves</topic><topic>Wave power</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Dinesh Kumar, E.</creatorcontrib><creatorcontrib>Sannasiraj, S. A.</creatorcontrib><creatorcontrib>Sundar, V.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physics of fluids (1994)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Dinesh Kumar, E.</au><au>Sannasiraj, S. A.</au><au>Sundar, V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Phase field lattice Boltzmann model for air-water two phase flows</atitle><jtitle>Physics of fluids (1994)</jtitle><date>2019-07</date><risdate>2019</risdate><volume>31</volume><issue>7</issue><issn>1070-6631</issn><eissn>1089-7666</eissn><coden>PHFLE6</coden><abstract>Two phase flows occur in different forms with liquid and gas in general, among which, the interaction of the flow of air and water is a common scenario. However, modeling the two phase flow still remains a challenge due to the large density ratio between them and different space-time scales involved in the flow regimes. In the present work, the lattice Boltzmann (LB) model capable of handling large density ratio (1000) and high Reynolds number (104) simultaneously is proposed. The present model consists of two sets of LB equations, one for the flow field in terms of normalized pressure-velocity formulation and the other for the solution of the conservative Allen-Cahn equation to capture the interface. The numerical tests such as stationary drop, bubble coalescence, and capillary wave decay have been performed, and the results exhibit excellent mass conservation property. The capability of the present model to handle complex scenarios has been tested through test cases, for example, rise of an air bubble, splash of a water droplet on a wet bed, and Rayleigh-Taylor instability. In all test cases, the simulation results agree well with the available reference data. Finally, as an application of the present model, the breaking of a deep water wave with high Reynolds number (104) is simulated. The plunging breaker with wave overturning and the generation of secondary jet and splashes are well described by the present LB model. The evolution of wave energy dissipation during and after breaking is in agreement with the reference data.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.5100215</doi><tpages>14</tpages><orcidid>https://orcid.org/0000-0002-5788-6696</orcidid><orcidid>https://orcid.org/0000-0003-4440-4771</orcidid><orcidid>https://orcid.org/0000-0001-7421-0543</orcidid></addata></record>
fulltext fulltext
identifier ISSN: 1070-6631
ispartof Physics of fluids (1994), 2019-07, Vol.31 (7)
issn 1070-6631
1089-7666
language eng
recordid cdi_proquest_journals_2255928040
source AIP Journals Complete; Alma/SFX Local Collection
subjects Aerodynamics
Air bubbles
Capillary waves
Coalescing
Computational fluid dynamics
Computer simulation
Deep water
Density ratio
Energy dissipation
Fluid dynamics
Fluid flow
High Reynolds number
Physics
Reynolds number
Taylor instability
Two phase flow
Water drops
Water waves
Wave power
title Phase field lattice Boltzmann model for air-water two phase flows
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-18T22%3A43%3A18IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_scita&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Phase%20field%20lattice%20Boltzmann%20model%20for%20air-water%20two%20phase%20flows&rft.jtitle=Physics%20of%20fluids%20(1994)&rft.au=Dinesh%20Kumar,%20E.&rft.date=2019-07&rft.volume=31&rft.issue=7&rft.issn=1070-6631&rft.eissn=1089-7666&rft.coden=PHFLE6&rft_id=info:doi/10.1063/1.5100215&rft_dat=%3Cproquest_scita%3E2255928040%3C/proquest_scita%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2255928040&rft_id=info:pmid/&rfr_iscdi=true