Barotropic instability of a zonal jet : From nondivergent perturbations on the β plane to divergent perturbations on a sphere
The linear instability of divergent perturbations that evolve on a cos2 mean steady zonal jet embedded in a zonal channel on the β plane and on a rotating sphere is studied for zonally propagating wavelike perturbations of the shallow-water equations. The complex phase speeds result from the imposit...
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description | The linear instability of divergent perturbations that evolve on a cos2 mean steady zonal jet embedded in a zonal channel on the β plane and on a rotating sphere is studied for zonally propagating wavelike perturbations of the shallow-water equations. The complex phase speeds result from the imposition of the no-flow boundary conditions at the channel walls on the numerical solutions of the linear differential equations for the wave latitude-dependent amplitude. In addition, the same numerical method is applied to the traditional problem of linear instability of nondivergent perturbations on the β plane where results reaffirm the classical, analytically derived, features. For these nondivergent perturbations, the present study shows that the growth rate increases monotonically with the jet maximal speed and that the classical result of a local maximum at some finite westward-directed speed results from scaling the growth rates on the jet’s speed. In contrast to nondivergent perturbations, divergent perturbations on the β plane have no short-wave cutoff, and so the nondivergent solution does not provide an estimate for the divergent solution, even when the ocean is 1000 km deep (i.e., when the speed of gravity waves exceeds 10 Mach). For realistic values of the ocean depth, the growth rates of divergent perturbations are smaller than those of nondivergent perturbations, but with the increase in the ocean depth they become larger than those of nondivergent perturbations. For both perturbations, a slight asymmetry exists between eastward- and westward-flowing jets. The growth rates of divergent perturbations on a sphere are similar to those on the β plane for the same values of the model parameters, but the asymmetry between eastward and westward jets is more conspicuous on a sphere. The value of g′H′ (g′ is the reduced gravity; H′ is the equivalent mean layer thickness), which is filtered out in nondivergent theory, determines for divergent perturbations the relative magnitude of zonal velocity, meridional velocity, and height but has little effect on the growth rates. |
doi_str_mv | 10.1175/JPO2960.1 |
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The complex phase speeds result from the imposition of the no-flow boundary conditions at the channel walls on the numerical solutions of the linear differential equations for the wave latitude-dependent amplitude. In addition, the same numerical method is applied to the traditional problem of linear instability of nondivergent perturbations on the β plane where results reaffirm the classical, analytically derived, features. For these nondivergent perturbations, the present study shows that the growth rate increases monotonically with the jet maximal speed and that the classical result of a local maximum at some finite westward-directed speed results from scaling the growth rates on the jet’s speed. In contrast to nondivergent perturbations, divergent perturbations on the β plane have no short-wave cutoff, and so the nondivergent solution does not provide an estimate for the divergent solution, even when the ocean is 1000 km deep (i.e., when the speed of gravity waves exceeds 10 Mach). For realistic values of the ocean depth, the growth rates of divergent perturbations are smaller than those of nondivergent perturbations, but with the increase in the ocean depth they become larger than those of nondivergent perturbations. For both perturbations, a slight asymmetry exists between eastward- and westward-flowing jets. The growth rates of divergent perturbations on a sphere are similar to those on the β plane for the same values of the model parameters, but the asymmetry between eastward and westward jets is more conspicuous on a sphere. The value of g′H′ (g′ is the reduced gravity; H′ is the equivalent mean layer thickness), which is filtered out in nondivergent theory, determines for divergent perturbations the relative magnitude of zonal velocity, meridional velocity, and height but has little effect on the growth rates.</description><identifier>ISSN: 0022-3670</identifier><identifier>EISSN: 1520-0485</identifier><identifier>DOI: 10.1175/JPO2960.1</identifier><identifier>CODEN: JPYOBT</identifier><language>eng</language><publisher>Boston, MA: American Meteorological Society</publisher><subject>Asymmetry ; Barotropic instability ; Barotropic mode ; Boundary conditions ; Differential equations ; Dynamics of the ocean (upper and deep oceans) ; Earth, ocean, space ; Eigenvalues ; Exact sciences and technology ; External geophysics ; Gravity waves ; Growth rate ; Instability ; Marine ; Mathematical models ; Microgravity ; Numerical methods ; Oceans ; Perturbation ; Perturbations ; Phase velocity ; Physics of the oceans ; Rotating spheres ; Scaling ; Shallow water ; Shallow water equations ; Stability ; Thickness ; Velocity ; Wave propagation</subject><ispartof>Journal of physical oceanography, 2006-12, Vol.36 (12), p.2271-2282</ispartof><rights>2007 INIST-CNRS</rights><rights>Copyright American Meteorological Society 2006</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c353t-fe1ff3b5cba0746cf316bb94888696dd20210360eeea2245542472d8f799a3c13</citedby><cites>FETCH-LOGICAL-c353t-fe1ff3b5cba0746cf316bb94888696dd20210360eeea2245542472d8f799a3c13</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,3681,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=18386031$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>PALDOR, Nathan</creatorcontrib><creatorcontrib>DVORKIN, Yona</creatorcontrib><title>Barotropic instability of a zonal jet : From nondivergent perturbations on the β plane to divergent perturbations on a sphere</title><title>Journal of physical oceanography</title><description>The linear instability of divergent perturbations that evolve on a cos2 mean steady zonal jet embedded in a zonal channel on the β plane and on a rotating sphere is studied for zonally propagating wavelike perturbations of the shallow-water equations. The complex phase speeds result from the imposition of the no-flow boundary conditions at the channel walls on the numerical solutions of the linear differential equations for the wave latitude-dependent amplitude. In addition, the same numerical method is applied to the traditional problem of linear instability of nondivergent perturbations on the β plane where results reaffirm the classical, analytically derived, features. For these nondivergent perturbations, the present study shows that the growth rate increases monotonically with the jet maximal speed and that the classical result of a local maximum at some finite westward-directed speed results from scaling the growth rates on the jet’s speed. In contrast to nondivergent perturbations, divergent perturbations on the β plane have no short-wave cutoff, and so the nondivergent solution does not provide an estimate for the divergent solution, even when the ocean is 1000 km deep (i.e., when the speed of gravity waves exceeds 10 Mach). For realistic values of the ocean depth, the growth rates of divergent perturbations are smaller than those of nondivergent perturbations, but with the increase in the ocean depth they become larger than those of nondivergent perturbations. For both perturbations, a slight asymmetry exists between eastward- and westward-flowing jets. The growth rates of divergent perturbations on a sphere are similar to those on the β plane for the same values of the model parameters, but the asymmetry between eastward and westward jets is more conspicuous on a sphere. The value of g′H′ (g′ is the reduced gravity; H′ is the equivalent mean layer thickness), which is filtered out in nondivergent theory, determines for divergent perturbations the relative magnitude of zonal velocity, meridional velocity, and height but has little effect on the growth rates.</description><subject>Asymmetry</subject><subject>Barotropic instability</subject><subject>Barotropic mode</subject><subject>Boundary conditions</subject><subject>Differential equations</subject><subject>Dynamics of the ocean (upper and deep oceans)</subject><subject>Earth, ocean, space</subject><subject>Eigenvalues</subject><subject>Exact sciences and technology</subject><subject>External geophysics</subject><subject>Gravity waves</subject><subject>Growth rate</subject><subject>Instability</subject><subject>Marine</subject><subject>Mathematical models</subject><subject>Microgravity</subject><subject>Numerical methods</subject><subject>Oceans</subject><subject>Perturbation</subject><subject>Perturbations</subject><subject>Phase velocity</subject><subject>Physics of the oceans</subject><subject>Rotating spheres</subject><subject>Scaling</subject><subject>Shallow water</subject><subject>Shallow water equations</subject><subject>Stability</subject><subject>Thickness</subject><subject>Velocity</subject><subject>Wave propagation</subject><issn>0022-3670</issn><issn>1520-0485</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><sourceid>8G5</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><sourceid>GUQSH</sourceid><sourceid>M2O</sourceid><recordid>eNp9kc1KAzEUhYMoWKsL3yAgCi5Gb5KZTMadFusPhbrQ9ZBJE5syTcYkFerCh_JBfCZbWhBcuLpc-O45l3MQOiZwQUhZXD4-jWnFV8sO6pGCQga5KHZRD4DSjPES9tFBjDMA4IRWPfR5I4NPwXdWYetiko1tbVpib7DEH97JFs90wld4GPwcO-8m9l2HV-0S7nRIi9DIZL2L2Ducphp_f-GulU7j5PE_qMSxm-qgD9GekW3UR9vZRy_D2-fBfTYa3z0MrkeZYgVLmdHEGNYUqpFQ5lwZRnjTVLkQgld8MqFACTAOWmtJaV4UOc1LOhGmrCrJFGF9dLbR7YJ_W-iY6rmNSrfrV_0i1qTipBSVWIEnf8CZX4RVDLGmAqAogVG-os43lAo-xqBN3QU7l2FZE6jXPdTbHuq19elWUUYlWxOkUzb-HggmODDCfgDGNIjv</recordid><startdate>20061201</startdate><enddate>20061201</enddate><creator>PALDOR, Nathan</creator><creator>DVORKIN, Yona</creator><general>American Meteorological Society</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7TG</scope><scope>7TN</scope><scope>7XB</scope><scope>88F</scope><scope>88I</scope><scope>8AF</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>8G5</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>ATCPS</scope><scope>AZQEC</scope><scope>BEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>F1W</scope><scope>GNUQQ</scope><scope>GUQSH</scope><scope>H96</scope><scope>HCIFZ</scope><scope>KL.</scope><scope>L.G</scope><scope>M1Q</scope><scope>M2O</scope><scope>M2P</scope><scope>MBDVC</scope><scope>P5Z</scope><scope>P62</scope><scope>PATMY</scope><scope>PCBAR</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PYCSY</scope><scope>Q9U</scope><scope>S0X</scope></search><sort><creationdate>20061201</creationdate><title>Barotropic instability of a zonal jet : From nondivergent perturbations on the β plane to divergent perturbations on a sphere</title><author>PALDOR, Nathan ; DVORKIN, Yona</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c353t-fe1ff3b5cba0746cf316bb94888696dd20210360eeea2245542472d8f799a3c13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2006</creationdate><topic>Asymmetry</topic><topic>Barotropic instability</topic><topic>Barotropic mode</topic><topic>Boundary conditions</topic><topic>Differential equations</topic><topic>Dynamics of the ocean (upper and deep oceans)</topic><topic>Earth, ocean, space</topic><topic>Eigenvalues</topic><topic>Exact sciences and technology</topic><topic>External geophysics</topic><topic>Gravity waves</topic><topic>Growth rate</topic><topic>Instability</topic><topic>Marine</topic><topic>Mathematical models</topic><topic>Microgravity</topic><topic>Numerical methods</topic><topic>Oceans</topic><topic>Perturbation</topic><topic>Perturbations</topic><topic>Phase velocity</topic><topic>Physics of the oceans</topic><topic>Rotating spheres</topic><topic>Scaling</topic><topic>Shallow water</topic><topic>Shallow water equations</topic><topic>Stability</topic><topic>Thickness</topic><topic>Velocity</topic><topic>Wave propagation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>PALDOR, Nathan</creatorcontrib><creatorcontrib>DVORKIN, Yona</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Oceanic Abstracts</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Military Database (Alumni Edition)</collection><collection>Science Database (Alumni Edition)</collection><collection>STEM Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>Research Library (Alumni Edition)</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>Agricultural & Environmental Science Collection</collection><collection>ProQuest Central Essentials</collection><collection>eLibrary</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>Natural Science Collection</collection><collection>Earth, Atmospheric & Aquatic Science Collection</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>Research Library Prep</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>Military Database</collection><collection>Research Library</collection><collection>Science Database</collection><collection>Research Library (Corporate)</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Environmental 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>Environmental Science Collection</collection><collection>ProQuest Central Basic</collection><collection>SIRS Editorial</collection><jtitle>Journal of physical oceanography</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>PALDOR, Nathan</au><au>DVORKIN, Yona</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Barotropic instability of a zonal jet : From nondivergent perturbations on the β plane to divergent perturbations on a sphere</atitle><jtitle>Journal of physical oceanography</jtitle><date>2006-12-01</date><risdate>2006</risdate><volume>36</volume><issue>12</issue><spage>2271</spage><epage>2282</epage><pages>2271-2282</pages><issn>0022-3670</issn><eissn>1520-0485</eissn><coden>JPYOBT</coden><abstract>The linear instability of divergent perturbations that evolve on a cos2 mean steady zonal jet embedded in a zonal channel on the β plane and on a rotating sphere is studied for zonally propagating wavelike perturbations of the shallow-water equations. The complex phase speeds result from the imposition of the no-flow boundary conditions at the channel walls on the numerical solutions of the linear differential equations for the wave latitude-dependent amplitude. In addition, the same numerical method is applied to the traditional problem of linear instability of nondivergent perturbations on the β plane where results reaffirm the classical, analytically derived, features. For these nondivergent perturbations, the present study shows that the growth rate increases monotonically with the jet maximal speed and that the classical result of a local maximum at some finite westward-directed speed results from scaling the growth rates on the jet’s speed. In contrast to nondivergent perturbations, divergent perturbations on the β plane have no short-wave cutoff, and so the nondivergent solution does not provide an estimate for the divergent solution, even when the ocean is 1000 km deep (i.e., when the speed of gravity waves exceeds 10 Mach). For realistic values of the ocean depth, the growth rates of divergent perturbations are smaller than those of nondivergent perturbations, but with the increase in the ocean depth they become larger than those of nondivergent perturbations. For both perturbations, a slight asymmetry exists between eastward- and westward-flowing jets. The growth rates of divergent perturbations on a sphere are similar to those on the β plane for the same values of the model parameters, but the asymmetry between eastward and westward jets is more conspicuous on a sphere. The value of g′H′ (g′ is the reduced gravity; H′ is the equivalent mean layer thickness), which is filtered out in nondivergent theory, determines for divergent perturbations the relative magnitude of zonal velocity, meridional velocity, and height but has little effect on the growth rates.</abstract><cop>Boston, MA</cop><pub>American Meteorological Society</pub><doi>10.1175/JPO2960.1</doi><tpages>12</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Asymmetry Barotropic instability Barotropic mode Boundary conditions Differential equations Dynamics of the ocean (upper and deep oceans) Earth, ocean, space Eigenvalues Exact sciences and technology External geophysics Gravity waves Growth rate Instability Marine Mathematical models Microgravity Numerical methods Oceans Perturbation Perturbations Phase velocity Physics of the oceans Rotating spheres Scaling Shallow water Shallow water equations Stability Thickness Velocity Wave propagation |
title | Barotropic instability of a zonal jet : From nondivergent perturbations on the β plane to divergent perturbations on a sphere |
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