Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow
In the frame of a three-layer quasi-geostrophic analytical model of a \(f\)-plane geophysical flow, Lagrangian advection being induced by the interaction of a monopole vortex with an isolated topographic feature is addressed. Two different cases when the monopole locates either within the upper or t...
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description | In the frame of a three-layer quasi-geostrophic analytical model of a \(f\)-plane geophysical flow, Lagrangian advection being induced by the interaction of a monopole vortex with an isolated topographic feature is addressed. Two different cases when the monopole locates either within the upper or the middle layer are of our interest. In the bottom layer, there is a delta function topographic feature, which generates a closed recirculation region in its vicinity due to the background flow. This recirculation region extends to the middle and upper layers, and it plays the role of a topographic vortex. The interaction between the monopole and the topographic vortex causes complex, including chaotic, advection of fluid particles. We show that the model's parameters, namely, the monopole and topographic vortices' strengths and initial positions, the layers' depths and densities are responsible for the diverse advection patterns. While the patterns are rather complicated, however, one can single out two major processes, which mostly govern fluid particle advection. The first one is the variation in time of the system's phase space structure, so that within the closed region of the topographic vortex, there appear periodically unclosed particle pathways by which the particles leave the topographic vortex. The second one is chaotic advection that arises from the nonstationarity of the monopole-topography interaction. |
doi_str_mv | 10.48550/arxiv.1209.6110 |
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Two different cases when the monopole locates either within the upper or the middle layer are of our interest. In the bottom layer, there is a delta function topographic feature, which generates a closed recirculation region in its vicinity due to the background flow. This recirculation region extends to the middle and upper layers, and it plays the role of a topographic vortex. The interaction between the monopole and the topographic vortex causes complex, including chaotic, advection of fluid particles. We show that the model's parameters, namely, the monopole and topographic vortices' strengths and initial positions, the layers' depths and densities are responsible for the diverse advection patterns. While the patterns are rather complicated, however, one can single out two major processes, which mostly govern fluid particle advection. The first one is the variation in time of the system's phase space structure, so that within the closed region of the topographic vortex, there appear periodically unclosed particle pathways by which the particles leave the topographic vortex. The second one is chaotic advection that arises from the nonstationarity of the monopole-topography interaction.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1209.6110</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Advection ; Computational fluid dynamics ; Delta function ; Fluid flow ; Geophysics ; Mathematical models ; Monopoles ; Physics - Atmospheric and Oceanic Physics ; Physics - Chaotic Dynamics ; Physics - Fluid Dynamics ; Topography ; Vortices</subject><ispartof>arXiv.org, 2012-09</ispartof><rights>2012. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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Two different cases when the monopole locates either within the upper or the middle layer are of our interest. In the bottom layer, there is a delta function topographic feature, which generates a closed recirculation region in its vicinity due to the background flow. This recirculation region extends to the middle and upper layers, and it plays the role of a topographic vortex. The interaction between the monopole and the topographic vortex causes complex, including chaotic, advection of fluid particles. We show that the model's parameters, namely, the monopole and topographic vortices' strengths and initial positions, the layers' depths and densities are responsible for the diverse advection patterns. While the patterns are rather complicated, however, one can single out two major processes, which mostly govern fluid particle advection. The first one is the variation in time of the system's phase space structure, so that within the closed region of the topographic vortex, there appear periodically unclosed particle pathways by which the particles leave the topographic vortex. The second one is chaotic advection that arises from the nonstationarity of the monopole-topography interaction.</description><subject>Advection</subject><subject>Computational fluid dynamics</subject><subject>Delta function</subject><subject>Fluid flow</subject><subject>Geophysics</subject><subject>Mathematical models</subject><subject>Monopoles</subject><subject>Physics - Atmospheric and Oceanic Physics</subject><subject>Physics - Chaotic Dynamics</subject><subject>Physics - Fluid Dynamics</subject><subject>Topography</subject><subject>Vortices</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotkDtrwzAUhUWh0JBm71QEnZ3qYUn2WEIfgUCX7ObavooVHMuVlYf_fZ2m0xnOg8NHyBNnyzRTir1CuLjTkguWLzXn7I7MhJQ8yVIhHshiGPaMMaGNUErOyG7dRQxQRec76i0FevCd732L9ORDxAs9u9hQ6KgbfAsRaxonexegb1xFLUI8BqSum5qxCYhJCyMGukPfN-PgKmipbf35kdxbaAdc_OucbD_et6uvZPP9uV69bRJQXCa1LiudZ8aYjDNRS6wMSmM1QI5pzdGmptaMW1PlVgJKhqUVJTMlyyymqOWcPN9m_yAUfXAHCGNxhVFcYUyBl1ugD_7niEMs9v4YuulSIVgmslQxJeUvdkBj_w</recordid><startdate>20120927</startdate><enddate>20120927</enddate><creator>Ryzhov, Evgeny A</creator><creator>Koshel, K V</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>ALA</scope><scope>GOX</scope></search><sort><creationdate>20120927</creationdate><title>Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow</title><author>Ryzhov, Evgeny A ; Koshel, K V</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a513-d6bc6987778102d3ec7e37f6aa9e4d1ef47d601f7c9f3ae30ebf2b07b08fe4e63</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Advection</topic><topic>Computational fluid dynamics</topic><topic>Delta function</topic><topic>Fluid flow</topic><topic>Geophysics</topic><topic>Mathematical models</topic><topic>Monopoles</topic><topic>Physics - Atmospheric and Oceanic Physics</topic><topic>Physics - Chaotic Dynamics</topic><topic>Physics - Fluid Dynamics</topic><topic>Topography</topic><topic>Vortices</topic><toplevel>online_resources</toplevel><creatorcontrib>Ryzhov, Evgeny A</creatorcontrib><creatorcontrib>Koshel, K V</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Access via ProQuest (Open Access)</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 China</collection><collection>Engineering Collection</collection><collection>arXiv Nonlinear Science</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ryzhov, Evgeny A</au><au>Koshel, K V</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow</atitle><jtitle>arXiv.org</jtitle><date>2012-09-27</date><risdate>2012</risdate><eissn>2331-8422</eissn><abstract>In the frame of a three-layer quasi-geostrophic analytical model of a \(f\)-plane geophysical flow, Lagrangian advection being induced by the interaction of a monopole vortex with an isolated topographic feature is addressed. Two different cases when the monopole locates either within the upper or the middle layer are of our interest. In the bottom layer, there is a delta function topographic feature, which generates a closed recirculation region in its vicinity due to the background flow. This recirculation region extends to the middle and upper layers, and it plays the role of a topographic vortex. The interaction between the monopole and the topographic vortex causes complex, including chaotic, advection of fluid particles. We show that the model's parameters, namely, the monopole and topographic vortices' strengths and initial positions, the layers' depths and densities are responsible for the diverse advection patterns. While the patterns are rather complicated, however, one can single out two major processes, which mostly govern fluid particle advection. The first one is the variation in time of the system's phase space structure, so that within the closed region of the topographic vortex, there appear periodically unclosed particle pathways by which the particles leave the topographic vortex. The second one is chaotic advection that arises from the nonstationarity of the monopole-topography interaction.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1209.6110</doi><oa>free_for_read</oa></addata></record> |
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subjects | Advection Computational fluid dynamics Delta function Fluid flow Geophysics Mathematical models Monopoles Physics - Atmospheric and Oceanic Physics Physics - Chaotic Dynamics Physics - Fluid Dynamics Topography Vortices |
title | Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow |
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