Surface‐layer description under free‐convection conditions
Large‐eddy simulation is used to study the structure of the boundary layer close to the surface under free‐convection conditions. The magnitude of the surface friction velocity induced by the large convective eddies is determined as a function of the convective velocity scale, w*, and the surface, r...
Gespeichert in:
Veröffentlicht in: | Quarterly journal of the Royal Meteorological Society 1993-04, Vol.119 (511), p.409-421 |
---|---|
Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 421 |
---|---|
container_issue | 511 |
container_start_page | 409 |
container_title | Quarterly journal of the Royal Meteorological Society |
container_volume | 119 |
creator | Sykes, R. I. Henn, D. S. Lewellen, W. S. |
description | Large‐eddy simulation is used to study the structure of the boundary layer close to the surface under free‐convection conditions. The magnitude of the surface friction velocity induced by the large convective eddies is determined as a function of the convective velocity scale, w*, and the surface, roughness length, z0. A simple analytic scaling form is obtained from a balance of forces in the wall layer induced by the convective eddies, giving the effective thickness of the layer and the effective surface stress and temperature dependence. The depth of the wall layer varies significantly with surface roughness and is extremely thin for small roughness, e.g. 0.5% of the mixed layer depth for a roughness length of 10−4zi. The analytic forms are consistent with the numerical predictions over the range of roughness length considered. The probability distribution of the instantaneous surface friction velocity (magnitude only) is examined and found to be reasonably close to Gaussian. |
doi_str_mv | 10.1002/qj.49711951103 |
format | Article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_18223229</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>18223229</sourcerecordid><originalsourceid>FETCH-LOGICAL-c4133-fdfca0885041f813a7fc59a8b386c2f9ba016f321b344c128faac51a0e611b023</originalsourceid><addsrcrecordid>eNqFkM1KAzEUhYMoWKtb112Iu6n35qdJNoIUfymIqOAuZDIJTJnOtElH6c5H8Bl9Eqe2SHeu7uHe75wLh5BThCEC0IvFdMi1RNQCEdge6SGXMlMS3vZJD4CJTAPoQ3KU0hQAhKSyRy6f2xis89-fX5Vd-TgofHKxnC_Lph60ddFtQvTrs2vqd-9-950syrVKx-Qg2Cr5k-3sk9eb65fxXTZ5vL0fX00yx5GxLBTBWVBKAMegkFkZnNBW5UyNHA06t4CjwCjmjHOHVAVrnUALfoSYA2V9cr7Jncdm0fq0NLMyOV9VtvZNmwwqShmlugOHG9DFJqXog5nHcmbjyiCYdU1mMTU7NXWGs22yTc5WIdralenPxaXQmkOH6Q32UVZ-9U-oeXrYffEDpsB6Mg</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>18223229</pqid></control><display><type>article</type><title>Surface‐layer description under free‐convection conditions</title><source>Wiley Online Library Journals Frontfile Complete</source><creator>Sykes, R. I. ; Henn, D. S. ; Lewellen, W. S.</creator><creatorcontrib>Sykes, R. I. ; Henn, D. S. ; Lewellen, W. S.</creatorcontrib><description>Large‐eddy simulation is used to study the structure of the boundary layer close to the surface under free‐convection conditions. The magnitude of the surface friction velocity induced by the large convective eddies is determined as a function of the convective velocity scale, w*, and the surface, roughness length, z0. A simple analytic scaling form is obtained from a balance of forces in the wall layer induced by the convective eddies, giving the effective thickness of the layer and the effective surface stress and temperature dependence. The depth of the wall layer varies significantly with surface roughness and is extremely thin for small roughness, e.g. 0.5% of the mixed layer depth for a roughness length of 10−4zi. The analytic forms are consistent with the numerical predictions over the range of roughness length considered. The probability distribution of the instantaneous surface friction velocity (magnitude only) is examined and found to be reasonably close to Gaussian.</description><identifier>ISSN: 0035-9009</identifier><identifier>EISSN: 1477-870X</identifier><identifier>DOI: 10.1002/qj.49711951103</identifier><identifier>CODEN: QJRMAM</identifier><language>eng</language><publisher>Bracknell: John Wiley & Sons, Ltd</publisher><subject>Convection, turbulence, diffusion. Boundary layer structure and dynamics ; Earth, ocean, space ; Exact sciences and technology ; External geophysics ; Meteorology</subject><ispartof>Quarterly journal of the Royal Meteorological Society, 1993-04, Vol.119 (511), p.409-421</ispartof><rights>Copyright © 1993 Royal Meteorological Society</rights><rights>1993 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4133-fdfca0885041f813a7fc59a8b386c2f9ba016f321b344c128faac51a0e611b023</citedby><cites>FETCH-LOGICAL-c4133-fdfca0885041f813a7fc59a8b386c2f9ba016f321b344c128faac51a0e611b023</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fqj.49711951103$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fqj.49711951103$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,27923,27924,45573,45574</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=4759940$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Sykes, R. I.</creatorcontrib><creatorcontrib>Henn, D. S.</creatorcontrib><creatorcontrib>Lewellen, W. S.</creatorcontrib><title>Surface‐layer description under free‐convection conditions</title><title>Quarterly journal of the Royal Meteorological Society</title><description>Large‐eddy simulation is used to study the structure of the boundary layer close to the surface under free‐convection conditions. The magnitude of the surface friction velocity induced by the large convective eddies is determined as a function of the convective velocity scale, w*, and the surface, roughness length, z0. A simple analytic scaling form is obtained from a balance of forces in the wall layer induced by the convective eddies, giving the effective thickness of the layer and the effective surface stress and temperature dependence. The depth of the wall layer varies significantly with surface roughness and is extremely thin for small roughness, e.g. 0.5% of the mixed layer depth for a roughness length of 10−4zi. The analytic forms are consistent with the numerical predictions over the range of roughness length considered. The probability distribution of the instantaneous surface friction velocity (magnitude only) is examined and found to be reasonably close to Gaussian.</description><subject>Convection, turbulence, diffusion. Boundary layer structure and dynamics</subject><subject>Earth, ocean, space</subject><subject>Exact sciences and technology</subject><subject>External geophysics</subject><subject>Meteorology</subject><issn>0035-9009</issn><issn>1477-870X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1993</creationdate><recordtype>article</recordtype><recordid>eNqFkM1KAzEUhYMoWKtb112Iu6n35qdJNoIUfymIqOAuZDIJTJnOtElH6c5H8Bl9Eqe2SHeu7uHe75wLh5BThCEC0IvFdMi1RNQCEdge6SGXMlMS3vZJD4CJTAPoQ3KU0hQAhKSyRy6f2xis89-fX5Vd-TgofHKxnC_Lph60ddFtQvTrs2vqd-9-950syrVKx-Qg2Cr5k-3sk9eb65fxXTZ5vL0fX00yx5GxLBTBWVBKAMegkFkZnNBW5UyNHA06t4CjwCjmjHOHVAVrnUALfoSYA2V9cr7Jncdm0fq0NLMyOV9VtvZNmwwqShmlugOHG9DFJqXog5nHcmbjyiCYdU1mMTU7NXWGs22yTc5WIdralenPxaXQmkOH6Q32UVZ-9U-oeXrYffEDpsB6Mg</recordid><startdate>199304</startdate><enddate>199304</enddate><creator>Sykes, R. I.</creator><creator>Henn, D. S.</creator><creator>Lewellen, W. S.</creator><general>John Wiley & Sons, Ltd</general><general>Wiley</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>KL.</scope></search><sort><creationdate>199304</creationdate><title>Surface‐layer description under free‐convection conditions</title><author>Sykes, R. I. ; Henn, D. S. ; Lewellen, W. S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4133-fdfca0885041f813a7fc59a8b386c2f9ba016f321b344c128faac51a0e611b023</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1993</creationdate><topic>Convection, turbulence, diffusion. Boundary layer structure and dynamics</topic><topic>Earth, ocean, space</topic><topic>Exact sciences and technology</topic><topic>External geophysics</topic><topic>Meteorology</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sykes, R. I.</creatorcontrib><creatorcontrib>Henn, D. S.</creatorcontrib><creatorcontrib>Lewellen, W. S.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><jtitle>Quarterly journal of the Royal Meteorological Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sykes, R. I.</au><au>Henn, D. S.</au><au>Lewellen, W. S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Surface‐layer description under free‐convection conditions</atitle><jtitle>Quarterly journal of the Royal Meteorological Society</jtitle><date>1993-04</date><risdate>1993</risdate><volume>119</volume><issue>511</issue><spage>409</spage><epage>421</epage><pages>409-421</pages><issn>0035-9009</issn><eissn>1477-870X</eissn><coden>QJRMAM</coden><abstract>Large‐eddy simulation is used to study the structure of the boundary layer close to the surface under free‐convection conditions. The magnitude of the surface friction velocity induced by the large convective eddies is determined as a function of the convective velocity scale, w*, and the surface, roughness length, z0. A simple analytic scaling form is obtained from a balance of forces in the wall layer induced by the convective eddies, giving the effective thickness of the layer and the effective surface stress and temperature dependence. The depth of the wall layer varies significantly with surface roughness and is extremely thin for small roughness, e.g. 0.5% of the mixed layer depth for a roughness length of 10−4zi. The analytic forms are consistent with the numerical predictions over the range of roughness length considered. The probability distribution of the instantaneous surface friction velocity (magnitude only) is examined and found to be reasonably close to Gaussian.</abstract><cop>Bracknell</cop><pub>John Wiley & Sons, Ltd</pub><doi>10.1002/qj.49711951103</doi><tpages>13</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0035-9009 |
ispartof | Quarterly journal of the Royal Meteorological Society, 1993-04, Vol.119 (511), p.409-421 |
issn | 0035-9009 1477-870X |
language | eng |
recordid | cdi_proquest_miscellaneous_18223229 |
source | Wiley Online Library Journals Frontfile Complete |
subjects | Convection, turbulence, diffusion. Boundary layer structure and dynamics Earth, ocean, space Exact sciences and technology External geophysics Meteorology |
title | Surface‐layer description under free‐convection conditions |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-08T22%3A37%3A22IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Surface%E2%80%90layer%20description%20under%20free%E2%80%90convection%20conditions&rft.jtitle=Quarterly%20journal%20of%20the%20Royal%20Meteorological%20Society&rft.au=Sykes,%20R.%20I.&rft.date=1993-04&rft.volume=119&rft.issue=511&rft.spage=409&rft.epage=421&rft.pages=409-421&rft.issn=0035-9009&rft.eissn=1477-870X&rft.coden=QJRMAM&rft_id=info:doi/10.1002/qj.49711951103&rft_dat=%3Cproquest_cross%3E18223229%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=18223229&rft_id=info:pmid/&rfr_iscdi=true |