Barotropic vorticity balance of the North Atlantic subpolar gyre in an eddy-resolving model

The circulation in the North Atlantic subpolar gyre is complex and strongly influenced by the topography. The gyre dynamics are traditionally understood as the result of a topographic Sverdrup balance, which corresponds to a first-order balance between the planetary vorticity advection, the bottom p...

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Published in:Ocean Science
Main Authors: M. Le Corre, J. Gula, A.-M. Tréguier
Format: Article in Journal/Newspaper
Language:English
Published: Copernicus Publications 2020
Subjects:
Online Access:https://doi.org/10.5194/os-16-451-2020
https://doaj.org/article/308449237dc34df18e0d593a2a25f3b2
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author M. Le Corre
J. Gula
A.-M. Tréguier
author_facet M. Le Corre
J. Gula
A.-M. Tréguier
author_sort M. Le Corre
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container_start_page 451
container_title Ocean Science
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description The circulation in the North Atlantic subpolar gyre is complex and strongly influenced by the topography. The gyre dynamics are traditionally understood as the result of a topographic Sverdrup balance, which corresponds to a first-order balance between the planetary vorticity advection, the bottom pressure torque, and the wind stress curl. However, these dynamics have been studied mostly with non-eddy-resolving models and a crude representation of the bottom topography. Here we revisit the barotropic vorticity balance of the North Atlantic subpolar gyre using a new eddy-resolving simulation (with a grid space of ≈2 km ) with topography-following vertical coordinates to better represent the mesoscale turbulence and flow–topography interactions. Our findings highlight that, locally, there is a first-order balance between the bottom pressure torque and the nonlinear terms, albeit with a high degree of cancellation between them. However, balances integrated over different regions of the gyre – shelf, slope, and interior – still highlight the important role played by nonlinearities and bottom drag curls. In particular, the Sverdrup balance cannot describe the dynamics in the interior of the gyre. The main sources of cyclonic vorticity are nonlinear terms due to eddies generated along eastern boundary currents and time-mean nonlinear terms in the northwest corner. Our results suggest that a good representation of the mesoscale activity and a good positioning of mean currents are two important conditions for a better representation of the circulation in the North Atlantic subpolar gyre.
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spelling ftdoajarticles:oai:doaj.org/article:308449237dc34df18e0d593a2a25f3b2 2025-01-16T23:33:03+00:00 Barotropic vorticity balance of the North Atlantic subpolar gyre in an eddy-resolving model M. Le Corre J. Gula A.-M. Tréguier 2020-04-01T00:00:00Z https://doi.org/10.5194/os-16-451-2020 https://doaj.org/article/308449237dc34df18e0d593a2a25f3b2 EN eng Copernicus Publications https://www.ocean-sci.net/16/451/2020/os-16-451-2020.pdf https://doaj.org/toc/1812-0784 https://doaj.org/toc/1812-0792 doi:10.5194/os-16-451-2020 1812-0784 1812-0792 https://doaj.org/article/308449237dc34df18e0d593a2a25f3b2 Ocean Science, Vol 16, Pp 451-468 (2020) Geography. Anthropology. Recreation G Environmental sciences GE1-350 article 2020 ftdoajarticles https://doi.org/10.5194/os-16-451-2020 2022-12-31T02:04:28Z The circulation in the North Atlantic subpolar gyre is complex and strongly influenced by the topography. The gyre dynamics are traditionally understood as the result of a topographic Sverdrup balance, which corresponds to a first-order balance between the planetary vorticity advection, the bottom pressure torque, and the wind stress curl. However, these dynamics have been studied mostly with non-eddy-resolving models and a crude representation of the bottom topography. Here we revisit the barotropic vorticity balance of the North Atlantic subpolar gyre using a new eddy-resolving simulation (with a grid space of ≈2 km ) with topography-following vertical coordinates to better represent the mesoscale turbulence and flow–topography interactions. Our findings highlight that, locally, there is a first-order balance between the bottom pressure torque and the nonlinear terms, albeit with a high degree of cancellation between them. However, balances integrated over different regions of the gyre – shelf, slope, and interior – still highlight the important role played by nonlinearities and bottom drag curls. In particular, the Sverdrup balance cannot describe the dynamics in the interior of the gyre. The main sources of cyclonic vorticity are nonlinear terms due to eddies generated along eastern boundary currents and time-mean nonlinear terms in the northwest corner. Our results suggest that a good representation of the mesoscale activity and a good positioning of mean currents are two important conditions for a better representation of the circulation in the North Atlantic subpolar gyre. Article in Journal/Newspaper North Atlantic Directory of Open Access Journals: DOAJ Articles Curl ENVELOPE(-63.071,-63.071,-70.797,-70.797) Ocean Science 16 2 451 468
spellingShingle Geography. Anthropology. Recreation
G
Environmental sciences
GE1-350
M. Le Corre
J. Gula
A.-M. Tréguier
Barotropic vorticity balance of the North Atlantic subpolar gyre in an eddy-resolving model
title Barotropic vorticity balance of the North Atlantic subpolar gyre in an eddy-resolving model
title_full Barotropic vorticity balance of the North Atlantic subpolar gyre in an eddy-resolving model
title_fullStr Barotropic vorticity balance of the North Atlantic subpolar gyre in an eddy-resolving model
title_full_unstemmed Barotropic vorticity balance of the North Atlantic subpolar gyre in an eddy-resolving model
title_short Barotropic vorticity balance of the North Atlantic subpolar gyre in an eddy-resolving model
title_sort barotropic vorticity balance of the north atlantic subpolar gyre in an eddy-resolving model
topic Geography. Anthropology. Recreation
G
Environmental sciences
GE1-350
topic_facet Geography. Anthropology. Recreation
G
Environmental sciences
GE1-350
url https://doi.org/10.5194/os-16-451-2020
https://doaj.org/article/308449237dc34df18e0d593a2a25f3b2