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 an <i>f</i>-plane geophysical flow, the Lagrangian advection induced by the interaction of a monopole vortex with an isolated topographic feature is addressed. Two different cases when the monopole is lo...

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Main Authors: E. A. Ryzhov, K. V. Koshel
Format: Article
Language:English
Published: Copernicus Publications 2013-02-01
Series:Nonlinear Processes in Geophysics
Online Access:http://www.nonlin-processes-geophys.net/20/107/2013/npg-20-107-2013.pdf
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spelling doaj-110157f465884c4ea9355be4f3bdcaa22020-11-25T00:44:13ZengCopernicus PublicationsNonlinear Processes in Geophysics1023-58091607-79462013-02-0120110711910.5194/npg-20-107-2013Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flowE. A. RyzhovK. V. KoshelIn the frame of a three-layer, quasi-geostrophic analytical model of an <i>f</i>-plane geophysical flow, the Lagrangian advection induced by the interaction of a monopole vortex with an isolated topographic feature is addressed. Two different cases when the monopole is located 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 a complex, including chaotic, advection of fluid particles. We show that the model's parameters, namely the monopole and topographic vortices' strengths and initial positions, and the layers' depths and densities, are responsible for the diverse advection patterns. While the patterns are rather complicated, one can single out two major processes, which mostly govern the 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.http://www.nonlin-processes-geophys.net/20/107/2013/npg-20-107-2013.pdf
collection DOAJ
language English
format Article
sources DOAJ
author E. A. Ryzhov
K. V. Koshel
spellingShingle E. A. Ryzhov
K. V. Koshel
Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow
Nonlinear Processes in Geophysics
author_facet E. A. Ryzhov
K. V. Koshel
author_sort E. A. Ryzhov
title Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow
title_short Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow
title_full Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow
title_fullStr Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow
title_full_unstemmed Interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow
title_sort interaction of a monopole vortex with an isolated topographic feature in a three-layer geophysical flow
publisher Copernicus Publications
series Nonlinear Processes in Geophysics
issn 1023-5809
1607-7946
publishDate 2013-02-01
description In the frame of a three-layer, quasi-geostrophic analytical model of an <i>f</i>-plane geophysical flow, the Lagrangian advection induced by the interaction of a monopole vortex with an isolated topographic feature is addressed. Two different cases when the monopole is located 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 a complex, including chaotic, advection of fluid particles. We show that the model's parameters, namely the monopole and topographic vortices' strengths and initial positions, and the layers' depths and densities, are responsible for the diverse advection patterns. While the patterns are rather complicated, one can single out two major processes, which mostly govern the 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.
url http://www.nonlin-processes-geophys.net/20/107/2013/npg-20-107-2013.pdf
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