Bubble size distribution in surface wave breaking entraining process
From the similarity theorem,an expression of bubble population is derived as a function of the air entrainment rate,the turbulent kinetic energy (TKE) spectrum density and the surface tension.The bubble size spectrum that we obtain has a dependence of a-2.5+nd on the bubble radius,in which nd is pos...
Gespeichert in:
Veröffentlicht in: | Science China. Earth sciences 2007-11, Vol.50 (11), p.1754-1760 |
---|---|
Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 1760 |
---|---|
container_issue | 11 |
container_start_page | 1754 |
container_title | Science China. Earth sciences |
container_volume | 50 |
creator | Han, Lei Yuan, YeLi |
description | From the similarity theorem,an expression of bubble population is derived as a function of the air entrainment rate,the turbulent kinetic energy (TKE) spectrum density and the surface tension.The bubble size spectrum that we obtain has a dependence of a-2.5+nd on the bubble radius,in which nd is positive and dependent on the form of TKE spectrum within the viscous dissipation range.To relate the bubble population with wave parameters,an expression about the air entrainment rate is deduced by introducing two statistical relations to wave breaking.The bubble population vertical distribution is also derived,based on two assumptions from two typical observation results. |
doi_str_mv | 10.1007/s11430-007-0116-7 |
format | Article |
fullrecord | <record><control><sourceid>wanfang_jour_proqu</sourceid><recordid>TN_cdi_wanfang_journals_zgkx_ed200711015</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><cqvip_id>1000887545</cqvip_id><wanfj_id>zgkx_ed200711015</wanfj_id><sourcerecordid>zgkx_ed200711015</sourcerecordid><originalsourceid>FETCH-LOGICAL-c397t-f17908fd62d3de9267775e4cd0da0d27ea0182b93e8efc1e801df65aef6e267f3</originalsourceid><addsrcrecordid>eNp9kUtLxDAUhYsoKOoPcFdE1E01t2mTdOlbYcCNrkPa3IyZqelM0vqYX2_KDC5cmE0O5Du5l3OS5AjIBRDCLwNAQUkWZUYAWMa3kj0QrMpAVHw7asaLjFOgu8lhCDMSD40vOd9Lbq-Hum4xDXaFqbah97Yeetu51Lo0DN6oBtNP9YFp7VHNrZum6HqvrBvlwncNhnCQ7BjVBjzc3PvJ6_3dy81jNnl-eLq5mmQNrXifGeAVEUazXFONVc445yUWjSZaEZ1zVAREXlcUBZoGUBDQhpUKDcMIG7qfnK___VTOKDeVs27wLk6Uq-n8S6LOYwQABMqInq3RuOJywNDLdxsabFvlsBuCFCUteMUqEsnTf8k8RiwIExE8_gP-jueMxkQBaIRgDTW-C8GjkQtv35X_lkDkWJZclyVHOZYlefScbDxvnZsuY7CyVs3c2BZHCxGCl0VJfwCQQ5Hz</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>763038113</pqid></control><display><type>article</type><title>Bubble size distribution in surface wave breaking entraining process</title><source>Springer Online Journals Complete</source><source>Alma/SFX Local Collection</source><creator>Han, Lei ; Yuan, YeLi</creator><creatorcontrib>Han, Lei ; Yuan, YeLi</creatorcontrib><description>From the similarity theorem,an expression of bubble population is derived as a function of the air entrainment rate,the turbulent kinetic energy (TKE) spectrum density and the surface tension.The bubble size spectrum that we obtain has a dependence of a-2.5+nd on the bubble radius,in which nd is positive and dependent on the form of TKE spectrum within the viscous dissipation range.To relate the bubble population with wave parameters,an expression about the air entrainment rate is deduced by introducing two statistical relations to wave breaking.The bubble population vertical distribution is also derived,based on two assumptions from two typical observation results.</description><identifier>ISSN: 1674-7313</identifier><identifier>ISSN: 1006-9313</identifier><identifier>EISSN: 1869-1897</identifier><identifier>EISSN: 1862-2801</identifier><identifier>DOI: 10.1007/s11430-007-0116-7</identifier><language>eng</language><publisher>Dordrecht: Springer Nature B.V</publisher><subject>breaking,bubble ; Bubble barriers ; cloud,bubble ; Earth science ; Geophysics ; size ; spectrum ; Surface waves ; wave</subject><ispartof>Science China. Earth sciences, 2007-11, Vol.50 (11), p.1754-1760</ispartof><rights>Science in China Press 2007</rights><rights>Copyright © Wanfang Data Co. Ltd. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c397t-f17908fd62d3de9267775e4cd0da0d27ea0182b93e8efc1e801df65aef6e267f3</citedby><cites>FETCH-LOGICAL-c397t-f17908fd62d3de9267775e4cd0da0d27ea0182b93e8efc1e801df65aef6e267f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://image.cqvip.com/vip1000/qk/60111X/60111X.jpg</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Han, Lei</creatorcontrib><creatorcontrib>Yuan, YeLi</creatorcontrib><title>Bubble size distribution in surface wave breaking entraining process</title><title>Science China. Earth sciences</title><description>From the similarity theorem,an expression of bubble population is derived as a function of the air entrainment rate,the turbulent kinetic energy (TKE) spectrum density and the surface tension.The bubble size spectrum that we obtain has a dependence of a-2.5+nd on the bubble radius,in which nd is positive and dependent on the form of TKE spectrum within the viscous dissipation range.To relate the bubble population with wave parameters,an expression about the air entrainment rate is deduced by introducing two statistical relations to wave breaking.The bubble population vertical distribution is also derived,based on two assumptions from two typical observation results.</description><subject>breaking,bubble</subject><subject>Bubble barriers</subject><subject>cloud,bubble</subject><subject>Earth science</subject><subject>Geophysics</subject><subject>size</subject><subject>spectrum</subject><subject>Surface waves</subject><subject>wave</subject><issn>1674-7313</issn><issn>1006-9313</issn><issn>1869-1897</issn><issn>1862-2801</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><recordid>eNp9kUtLxDAUhYsoKOoPcFdE1E01t2mTdOlbYcCNrkPa3IyZqelM0vqYX2_KDC5cmE0O5Du5l3OS5AjIBRDCLwNAQUkWZUYAWMa3kj0QrMpAVHw7asaLjFOgu8lhCDMSD40vOd9Lbq-Hum4xDXaFqbah97Yeetu51Lo0DN6oBtNP9YFp7VHNrZum6HqvrBvlwncNhnCQ7BjVBjzc3PvJ6_3dy81jNnl-eLq5mmQNrXifGeAVEUazXFONVc445yUWjSZaEZ1zVAREXlcUBZoGUBDQhpUKDcMIG7qfnK___VTOKDeVs27wLk6Uq-n8S6LOYwQABMqInq3RuOJywNDLdxsabFvlsBuCFCUteMUqEsnTf8k8RiwIExE8_gP-jueMxkQBaIRgDTW-C8GjkQtv35X_lkDkWJZclyVHOZYlefScbDxvnZsuY7CyVs3c2BZHCxGCl0VJfwCQQ5Hz</recordid><startdate>20071101</startdate><enddate>20071101</enddate><creator>Han, Lei</creator><creator>Yuan, YeLi</creator><general>Springer Nature B.V</general><general>The First Institute of Oceanography,State Ocean Administration,Qingdao 266061,China%The First Institute of Oceanography,State Ocean Administration,Qingdao 266061,China</general><general>Department of Ocean Environment,Ocean University of China,Qingdao 266003,China</general><scope>2RA</scope><scope>92L</scope><scope>CQIGP</scope><scope>~WA</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7TG</scope><scope>7UA</scope><scope>7XB</scope><scope>88I</scope><scope>8FK</scope><scope>ABUWG</scope><scope>AEUYN</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>C1K</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>F1W</scope><scope>GNUQQ</scope><scope>H96</scope><scope>HCIFZ</scope><scope>KL.</scope><scope>L.G</scope><scope>M2P</scope><scope>PCBAR</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>Q9U</scope><scope>7TN</scope><scope>2B.</scope><scope>4A8</scope><scope>92I</scope><scope>93N</scope><scope>PSX</scope><scope>TCJ</scope></search><sort><creationdate>20071101</creationdate><title>Bubble size distribution in surface wave breaking entraining process</title><author>Han, Lei ; Yuan, YeLi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c397t-f17908fd62d3de9267775e4cd0da0d27ea0182b93e8efc1e801df65aef6e267f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2007</creationdate><topic>breaking,bubble</topic><topic>Bubble barriers</topic><topic>cloud,bubble</topic><topic>Earth science</topic><topic>Geophysics</topic><topic>size</topic><topic>spectrum</topic><topic>Surface waves</topic><topic>wave</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Han, Lei</creatorcontrib><creatorcontrib>Yuan, YeLi</creatorcontrib><collection>中文科技期刊数据库</collection><collection>中文科技期刊数据库-CALIS站点</collection><collection>中文科技期刊数据库-7.0平台</collection><collection>中文科技期刊数据库- 镜像站点</collection><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Water Resources Abstracts</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Science Database (Alumni Edition)</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest One Sustainability</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Natural Science Collection</collection><collection>Earth, Atmospheric & Aquatic Science Collection</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>ProQuest Central Student</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>SciTech Premium Collection</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Science Database</collection><collection>Earth, Atmospheric & Aquatic Science Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central Basic</collection><collection>Oceanic Abstracts</collection><collection>Wanfang Data Journals - Hong Kong</collection><collection>WANFANG Data Centre</collection><collection>Wanfang Data Journals</collection><collection>万方数据期刊 - 香港版</collection><collection>China Online Journals (COJ)</collection><collection>China Online Journals (COJ)</collection><jtitle>Science China. Earth sciences</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Han, Lei</au><au>Yuan, YeLi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Bubble size distribution in surface wave breaking entraining process</atitle><jtitle>Science China. Earth sciences</jtitle><date>2007-11-01</date><risdate>2007</risdate><volume>50</volume><issue>11</issue><spage>1754</spage><epage>1760</epage><pages>1754-1760</pages><issn>1674-7313</issn><issn>1006-9313</issn><eissn>1869-1897</eissn><eissn>1862-2801</eissn><abstract>From the similarity theorem,an expression of bubble population is derived as a function of the air entrainment rate,the turbulent kinetic energy (TKE) spectrum density and the surface tension.The bubble size spectrum that we obtain has a dependence of a-2.5+nd on the bubble radius,in which nd is positive and dependent on the form of TKE spectrum within the viscous dissipation range.To relate the bubble population with wave parameters,an expression about the air entrainment rate is deduced by introducing two statistical relations to wave breaking.The bubble population vertical distribution is also derived,based on two assumptions from two typical observation results.</abstract><cop>Dordrecht</cop><pub>Springer Nature B.V</pub><doi>10.1007/s11430-007-0116-7</doi><tpages>7</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 1674-7313 |
ispartof | Science China. Earth sciences, 2007-11, Vol.50 (11), p.1754-1760 |
issn | 1674-7313 1006-9313 1869-1897 1862-2801 |
language | eng |
recordid | cdi_wanfang_journals_zgkx_ed200711015 |
source | Springer Online Journals Complete; Alma/SFX Local Collection |
subjects | breaking,bubble Bubble barriers cloud,bubble Earth science Geophysics size spectrum Surface waves wave |
title | Bubble size distribution in surface wave breaking entraining process |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-11T01%3A38%3A00IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-wanfang_jour_proqu&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Bubble%20size%20distribution%20in%20surface%20wave%20breaking%20entraining%20process&rft.jtitle=Science%20China.%20Earth%20sciences&rft.au=Han,%20Lei&rft.date=2007-11-01&rft.volume=50&rft.issue=11&rft.spage=1754&rft.epage=1760&rft.pages=1754-1760&rft.issn=1674-7313&rft.eissn=1869-1897&rft_id=info:doi/10.1007/s11430-007-0116-7&rft_dat=%3Cwanfang_jour_proqu%3Ezgkx_ed200711015%3C/wanfang_jour_proqu%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=763038113&rft_id=info:pmid/&rft_cqvip_id=1000887545&rft_wanfj_id=zgkx_ed200711015&rfr_iscdi=true |