Convectively driven mixed layer growth in a rotating, stratified fluid
A laboratory experiment has been conducted to examine deep convective processes in a stratified ocean. For convenience, cooling at the ocean surface is modelled in the laboratory by heating from below. A convective mixed layer was generated by heating over the central portion of the base of a rotati...
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Veröffentlicht in: | Deep-sea research. Part I, Oceanographic research papers Oceanographic research papers, 1995, Vol.42 (3), p.331-349 |
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creator | Ivey, G.N. Taylor, J.R. Coates, M.J. |
description | A laboratory experiment has been conducted to examine deep convective processes in a stratified ocean. For convenience, cooling at the ocean surface is modelled in the laboratory by heating from below. A convective mixed layer was generated by heating over the central portion of the base of a rotating, thermally stratified fluid. In addition to the convective forcing, the initial stratification could also be pre-conditioned by rotating a false bottom in the tank, thus generating a cyclonic or anticyclonic initial circulation in the tank as desired. Following the initiation of the buoyancy flux, a mixed layer forms above the buoyancy source and erodes the overlying thermal stratification. Initially confined by rotation, the growth of the mixed layer depth with time is described by a one-dimensional deepening law. The front separating the heated convecting fluid from the stratified, quiescent ambient fluid eventually becomes unstable, generating a field of baroclinic eddies. The rate of deepening of the mixed layer slows as the eddy field develops and transports both buoyant fluid from above the source region horizontally into the unheated sections of the tank and ambient fluid horizontally into the source region. Ventilation of the deep and relatively unstratified water beyond the thermocline is thus most likely to occur if the thermocline is penetrated before the eddy field becomes fully developed. |
doi_str_mv | 10.1016/0967-0637(94)00039-U |
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For convenience, cooling at the ocean surface is modelled in the laboratory by heating from below. A convective mixed layer was generated by heating over the central portion of the base of a rotating, thermally stratified fluid. In addition to the convective forcing, the initial stratification could also be pre-conditioned by rotating a false bottom in the tank, thus generating a cyclonic or anticyclonic initial circulation in the tank as desired. Following the initiation of the buoyancy flux, a mixed layer forms above the buoyancy source and erodes the overlying thermal stratification. Initially confined by rotation, the growth of the mixed layer depth with time is described by a one-dimensional deepening law. The front separating the heated convecting fluid from the stratified, quiescent ambient fluid eventually becomes unstable, generating a field of baroclinic eddies. The rate of deepening of the mixed layer slows as the eddy field develops and transports both buoyant fluid from above the source region horizontally into the unheated sections of the tank and ambient fluid horizontally into the source region. Ventilation of the deep and relatively unstratified water beyond the thermocline is thus most likely to occur if the thermocline is penetrated before the eddy field becomes fully developed.</description><identifier>ISSN: 0967-0637</identifier><identifier>EISSN: 1879-0119</identifier><identifier>DOI: 10.1016/0967-0637(94)00039-U</identifier><language>eng</language><publisher>Oxford: Elsevier Ltd</publisher><subject>Dynamics of the ocean (upper and deep oceans) ; Earth, ocean, space ; Exact sciences and technology ; External geophysics ; Marine ; Oceanography ; Oceans ; Physics of the oceans</subject><ispartof>Deep-sea research. 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The front separating the heated convecting fluid from the stratified, quiescent ambient fluid eventually becomes unstable, generating a field of baroclinic eddies. The rate of deepening of the mixed layer slows as the eddy field develops and transports both buoyant fluid from above the source region horizontally into the unheated sections of the tank and ambient fluid horizontally into the source region. Ventilation of the deep and relatively unstratified water beyond the thermocline is thus most likely to occur if the thermocline is penetrated before the eddy field becomes fully developed.</description><subject>Dynamics of the ocean (upper and deep oceans)</subject><subject>Earth, ocean, space</subject><subject>Exact sciences and technology</subject><subject>External geophysics</subject><subject>Marine</subject><subject>Oceanography</subject><subject>Oceans</subject><subject>Physics of the oceans</subject><issn>0967-0637</issn><issn>1879-0119</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1995</creationdate><recordtype>article</recordtype><recordid>eNqFkU9PGzEQxa0KpIbAN-hhVVWoSF3wYK__XJCqiBQkJC7kbHntMTXa7FJ7kzbfHodEHHqA08zh995o3iPkC9BzoCAuqBaypoLJ75qfUUqZrhefyASU1DUF0Adk8oZ8Jkc5PxUIhKITMp8N_RrdGNfYbSqfyuyrZfyHvursBlP1mIa_4-8q9pWt0jDaMfaPP6o8prKFWLDQraI_JofBdhlP9nNKFvPrh9lNfXf_63b28652_PJyrFultEcfqAZtvYcAyMBjYBzQcuq0FFI5HnQrNGcoGnTIpWqb1rai4ZpNyenO9zkNf1aYR7OM2WHX2R6HVTagQEpg8mNQqEZxxgv49T_waVilvjxhQAuhhGC0QHwHuTTknDCY5xSXNm0MULOtwGzzNdt8jebmtQKzKLJve2-bne1Csr2L-U3LJJVN0UzJ1Q7Dktw6YjLZRewd-phKNcYP8f07L3Ajmeo</recordid><startdate>1995</startdate><enddate>1995</enddate><creator>Ivey, G.N.</creator><creator>Taylor, J.R.</creator><creator>Coates, M.J.</creator><general>Elsevier Ltd</general><general>Elsevier</general><general>Pergamon Press Inc</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TN</scope><scope>F1W</scope><scope>H96</scope><scope>L.G</scope><scope>7TG</scope><scope>KL.</scope></search><sort><creationdate>1995</creationdate><title>Convectively driven mixed layer growth in a rotating, stratified fluid</title><author>Ivey, G.N. ; Taylor, J.R. ; Coates, M.J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c422t-b889dedf0919add1f1e31def341ea40c97678c4f9b6943e65ece478b5bab65493</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1995</creationdate><topic>Dynamics of the ocean (upper and deep oceans)</topic><topic>Earth, ocean, space</topic><topic>Exact sciences and technology</topic><topic>External geophysics</topic><topic>Marine</topic><topic>Oceanography</topic><topic>Oceans</topic><topic>Physics of the oceans</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ivey, G.N.</creatorcontrib><creatorcontrib>Taylor, J.R.</creatorcontrib><creatorcontrib>Coates, M.J.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Oceanic Abstracts</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><jtitle>Deep-sea research. 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In addition to the convective forcing, the initial stratification could also be pre-conditioned by rotating a false bottom in the tank, thus generating a cyclonic or anticyclonic initial circulation in the tank as desired. Following the initiation of the buoyancy flux, a mixed layer forms above the buoyancy source and erodes the overlying thermal stratification. Initially confined by rotation, the growth of the mixed layer depth with time is described by a one-dimensional deepening law. The front separating the heated convecting fluid from the stratified, quiescent ambient fluid eventually becomes unstable, generating a field of baroclinic eddies. The rate of deepening of the mixed layer slows as the eddy field develops and transports both buoyant fluid from above the source region horizontally into the unheated sections of the tank and ambient fluid horizontally into the source region. Ventilation of the deep and relatively unstratified water beyond the thermocline is thus most likely to occur if the thermocline is penetrated before the eddy field becomes fully developed.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/0967-0637(94)00039-U</doi><tpages>19</tpages></addata></record> |
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source | Elsevier ScienceDirect Journals Complete |
subjects | Dynamics of the ocean (upper and deep oceans) Earth, ocean, space Exact sciences and technology External geophysics Marine Oceanography Oceans Physics of the oceans |
title | Convectively driven mixed layer growth in a rotating, stratified fluid |
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