Loading…

Transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel

An experimental study was conducted to investigate the transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel. Three experiments, with a reduced gravity of g' = 1.64, 6.47 and 18.0 cm s −2 , were performed. Particle image velocimetry and planar laser...

Full description

Saved in:
Bibliographic Details
Published in:Atmosphere-ocean 2008-12, Vol.46 (4), p.391-404
Main Authors: Fouli, Hesham, Zhu, David Z.
Format: Article
Language:English
Subjects:
Citations: Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c289t-d344e2937763312265676cfa2579c690ffd61a1c457481d3993c1cf9ea63297a3
cites
container_end_page 404
container_issue 4
container_start_page 391
container_title Atmosphere-ocean
container_volume 46
creator Fouli, Hesham
Zhu, David Z.
description An experimental study was conducted to investigate the transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel. Three experiments, with a reduced gravity of g' = 1.64, 6.47 and 18.0 cm s −2 , were performed. Particle image velocimetry and planar laser-induced fluorescence were used to obtain the measurements of velocity and concentration fields. The flow rate, obtained from the measured velocity field, increases significantly toward the toe of the topography by almost 40% from that at the sill crest due to the interfacial wave activities. In the horizontal channel, however, the flow rate only increases marginally. Estimates of the composite Froude number indicate that the supercritical flow on the slope of the topography goes through the transition to the subcritical flow in the horizontal channel. The transition is mainly due to the increase in the lower-layer thickness because of increasing interfacial friction caused by the breaking of interfacial waves, and no internal hydraulic jumps are observed. The measured mean concentration field showed the formation of an intermediate layer of medium density, which increased its thickness with g' and helped to suppress turbulence. Spectral analysis of the density interfacial fluctuations indicated that the interfacial waves that developed on the slope of the topography broke up downstream of the toe into smaller amplitude waves at larger frequencies. The waves at several channel cross-sections were also examined.
doi_str_mv 10.3137/ao.460401
format article
fullrecord <record><control><sourceid>pascalfrancis_cross</sourceid><recordid>TN_cdi_crossref_primary_10_3137_ao_460401</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>20966331</sourcerecordid><originalsourceid>FETCH-LOGICAL-c289t-d344e2937763312265676cfa2579c690ffd61a1c457481d3993c1cf9ea63297a3</originalsourceid><addsrcrecordid>eNplkE1LAzEQhoMoWKsH_0EuHjxszdcmzVGKX1DwUs_LmE3sSrqzJIFSf71bVr14mmF43pfhIeSas4Xk0twBLpRmivETMuNqySoruDolM2ZYXdWWsXNykfMnY4IZI2fEbRL0uSsd9hQDLXusIhx8orkkKF3ofEtDxD0NCXe0bD3NEQd_ZN-xlOMNB_xIMGwP40qBbjF1X9gXiNRtoe99vCRnAWL2Vz9zTt4eHzar52r9-vSyul9XTixtqVqplBdWGqOl5ELoWhvtAojaWKctC6HVHLhTtVFL3kprpeMuWA9aCmtAzsnt1OsS5px8aIbU7SAdGs6ao50GsJnsjOzNxA6QHcQwWnBd_gsIZvXxi5FTE9f1AdMO9phi2xQ4REy_Ifm__hsyE3bX</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel</title><source>Taylor and Francis Science and Technology Collection</source><creator>Fouli, Hesham ; Zhu, David Z.</creator><creatorcontrib>Fouli, Hesham ; Zhu, David Z.</creatorcontrib><description>An experimental study was conducted to investigate the transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel. Three experiments, with a reduced gravity of g' = 1.64, 6.47 and 18.0 cm s −2 , were performed. Particle image velocimetry and planar laser-induced fluorescence were used to obtain the measurements of velocity and concentration fields. The flow rate, obtained from the measured velocity field, increases significantly toward the toe of the topography by almost 40% from that at the sill crest due to the interfacial wave activities. In the horizontal channel, however, the flow rate only increases marginally. Estimates of the composite Froude number indicate that the supercritical flow on the slope of the topography goes through the transition to the subcritical flow in the horizontal channel. The transition is mainly due to the increase in the lower-layer thickness because of increasing interfacial friction caused by the breaking of interfacial waves, and no internal hydraulic jumps are observed. The measured mean concentration field showed the formation of an intermediate layer of medium density, which increased its thickness with g' and helped to suppress turbulence. Spectral analysis of the density interfacial fluctuations indicated that the interfacial waves that developed on the slope of the topography broke up downstream of the toe into smaller amplitude waves at larger frequencies. The waves at several channel cross-sections were also examined.</description><identifier>ISSN: 0705-5900</identifier><identifier>EISSN: 1480-9214</identifier><identifier>DOI: 10.3137/ao.460401</identifier><language>eng</language><publisher>Ottawa: Taylor &amp; Francis Group</publisher><subject>Earth, ocean, space ; Exact sciences and technology ; External geophysics ; Geophysics. Techniques, methods, instrumentation and models ; Meteorology ; Other topics ; Other topics in atmospheric geophysics ; Physics of the oceans</subject><ispartof>Atmosphere-ocean, 2008-12, Vol.46 (4), p.391-404</ispartof><rights>Copyright Taylor &amp; Francis Group, LLC 2008</rights><rights>2009 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c289t-d344e2937763312265676cfa2579c690ffd61a1c457481d3993c1cf9ea63297a3</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,780,784,789,790,23930,23931,25140,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=20966331$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Fouli, Hesham</creatorcontrib><creatorcontrib>Zhu, David Z.</creatorcontrib><title>Transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel</title><title>Atmosphere-ocean</title><description>An experimental study was conducted to investigate the transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel. Three experiments, with a reduced gravity of g' = 1.64, 6.47 and 18.0 cm s −2 , were performed. Particle image velocimetry and planar laser-induced fluorescence were used to obtain the measurements of velocity and concentration fields. The flow rate, obtained from the measured velocity field, increases significantly toward the toe of the topography by almost 40% from that at the sill crest due to the interfacial wave activities. In the horizontal channel, however, the flow rate only increases marginally. Estimates of the composite Froude number indicate that the supercritical flow on the slope of the topography goes through the transition to the subcritical flow in the horizontal channel. The transition is mainly due to the increase in the lower-layer thickness because of increasing interfacial friction caused by the breaking of interfacial waves, and no internal hydraulic jumps are observed. The measured mean concentration field showed the formation of an intermediate layer of medium density, which increased its thickness with g' and helped to suppress turbulence. Spectral analysis of the density interfacial fluctuations indicated that the interfacial waves that developed on the slope of the topography broke up downstream of the toe into smaller amplitude waves at larger frequencies. The waves at several channel cross-sections were also examined.</description><subject>Earth, ocean, space</subject><subject>Exact sciences and technology</subject><subject>External geophysics</subject><subject>Geophysics. Techniques, methods, instrumentation and models</subject><subject>Meteorology</subject><subject>Other topics</subject><subject>Other topics in atmospheric geophysics</subject><subject>Physics of the oceans</subject><issn>0705-5900</issn><issn>1480-9214</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNplkE1LAzEQhoMoWKsH_0EuHjxszdcmzVGKX1DwUs_LmE3sSrqzJIFSf71bVr14mmF43pfhIeSas4Xk0twBLpRmivETMuNqySoruDolM2ZYXdWWsXNykfMnY4IZI2fEbRL0uSsd9hQDLXusIhx8orkkKF3ofEtDxD0NCXe0bD3NEQd_ZN-xlOMNB_xIMGwP40qBbjF1X9gXiNRtoe99vCRnAWL2Vz9zTt4eHzar52r9-vSyul9XTixtqVqplBdWGqOl5ELoWhvtAojaWKctC6HVHLhTtVFL3kprpeMuWA9aCmtAzsnt1OsS5px8aIbU7SAdGs6ao50GsJnsjOzNxA6QHcQwWnBd_gsIZvXxi5FTE9f1AdMO9phi2xQ4REy_Ifm__hsyE3bX</recordid><startdate>20081201</startdate><enddate>20081201</enddate><creator>Fouli, Hesham</creator><creator>Zhu, David Z.</creator><general>Taylor &amp; Francis Group</general><general>Société canadienne de météorologie et d'océanographie</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20081201</creationdate><title>Transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel</title><author>Fouli, Hesham ; Zhu, David Z.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c289t-d344e2937763312265676cfa2579c690ffd61a1c457481d3993c1cf9ea63297a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><topic>Earth, ocean, space</topic><topic>Exact sciences and technology</topic><topic>External geophysics</topic><topic>Geophysics. Techniques, methods, instrumentation and models</topic><topic>Meteorology</topic><topic>Other topics</topic><topic>Other topics in atmospheric geophysics</topic><topic>Physics of the oceans</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Fouli, Hesham</creatorcontrib><creatorcontrib>Zhu, David Z.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Atmosphere-ocean</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Fouli, Hesham</au><au>Zhu, David Z.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel</atitle><jtitle>Atmosphere-ocean</jtitle><date>2008-12-01</date><risdate>2008</risdate><volume>46</volume><issue>4</issue><spage>391</spage><epage>404</epage><pages>391-404</pages><issn>0705-5900</issn><eissn>1480-9214</eissn><abstract>An experimental study was conducted to investigate the transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel. Three experiments, with a reduced gravity of g' = 1.64, 6.47 and 18.0 cm s −2 , were performed. Particle image velocimetry and planar laser-induced fluorescence were used to obtain the measurements of velocity and concentration fields. The flow rate, obtained from the measured velocity field, increases significantly toward the toe of the topography by almost 40% from that at the sill crest due to the interfacial wave activities. In the horizontal channel, however, the flow rate only increases marginally. Estimates of the composite Froude number indicate that the supercritical flow on the slope of the topography goes through the transition to the subcritical flow in the horizontal channel. The transition is mainly due to the increase in the lower-layer thickness because of increasing interfacial friction caused by the breaking of interfacial waves, and no internal hydraulic jumps are observed. The measured mean concentration field showed the formation of an intermediate layer of medium density, which increased its thickness with g' and helped to suppress turbulence. Spectral analysis of the density interfacial fluctuations indicated that the interfacial waves that developed on the slope of the topography broke up downstream of the toe into smaller amplitude waves at larger frequencies. The waves at several channel cross-sections were also examined.</abstract><cop>Ottawa</cop><pub>Taylor &amp; Francis Group</pub><doi>10.3137/ao.460401</doi><tpages>14</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0705-5900
ispartof Atmosphere-ocean, 2008-12, Vol.46 (4), p.391-404
issn 0705-5900
1480-9214
language eng
recordid cdi_crossref_primary_10_3137_ao_460401
source Taylor and Francis Science and Technology Collection
subjects Earth, ocean, space
Exact sciences and technology
External geophysics
Geophysics. Techniques, methods, instrumentation and models
Meteorology
Other topics
Other topics in atmospheric geophysics
Physics of the oceans
title Transition of two-layer stratified flow from the slope of bottom topography to a horizontal channel
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-27T18%3A55%3A33IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-pascalfrancis_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Transition%20of%20two-layer%20stratified%20flow%20from%20the%20slope%20of%20bottom%20topography%20to%20a%20horizontal%20channel&rft.jtitle=Atmosphere-ocean&rft.au=Fouli,%20Hesham&rft.date=2008-12-01&rft.volume=46&rft.issue=4&rft.spage=391&rft.epage=404&rft.pages=391-404&rft.issn=0705-5900&rft.eissn=1480-9214&rft_id=info:doi/10.3137/ao.460401&rft_dat=%3Cpascalfrancis_cross%3E20966331%3C/pascalfrancis_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c289t-d344e2937763312265676cfa2579c690ffd61a1c457481d3993c1cf9ea63297a3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true