Parameterization of eddy-induced subduction in the Southern Ocean surface-layer
The divergence of the eddy mass flux in the surface layer of the Southern Ocean makes an important contribution to subduction of fluid through the base of the mixed layer. Therefore, accurate parameterization of this process is needed to correctly represent the Southern Ocean ventilation in coarse-r...
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Online Access: | https://doi.org/10.1016/j.ocemod.2011.04.001 http://ecite.utas.edu.au/80635 |
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ftunivtasecite:oai:ecite.utas.edu.au:80635 2023-05-15T18:24:17+02:00 Parameterization of eddy-induced subduction in the Southern Ocean surface-layer Sallee, J-B Rintoul, SR 2011 https://doi.org/10.1016/j.ocemod.2011.04.001 http://ecite.utas.edu.au/80635 en eng Elsevier Sci Ltd http://dx.doi.org/10.1016/j.ocemod.2011.04.001 Sallee, J-B and Rintoul, SR, Parameterization of eddy-induced subduction in the Southern Ocean surface-layer, Ocean Modelling, 39, (1-2) pp. 146-153. ISSN 1463-5003 (2011) [Refereed Article] http://ecite.utas.edu.au/80635 Earth Sciences Oceanography Physical Oceanography Refereed Article PeerReviewed 2011 ftunivtasecite https://doi.org/10.1016/j.ocemod.2011.04.001 2019-12-13T21:45:53Z The divergence of the eddy mass flux in the surface layer of the Southern Ocean makes an important contribution to subduction of fluid through the base of the mixed layer. Therefore, accurate parameterization of this process is needed to correctly represent the Southern Ocean ventilation in coarse-resolution models. We test a common approach to the parameterization of eddy fluxes (Gent and McWilliams, 1990) using output from the 1/6 eddy-permitting Southern Ocean State Estimate, which assimilates a variety of ocean observations using an adjoint method. When a constant diffusion coefficient of conventional magnitude O(1000 m2 s−1) is used, the parameterized fluxes fail to reproduce the regional pattern and magnitude of eddy-driven subduction diagnosed from the model. However, when an appropriate choice is made for the diffusion coefficient, the parameterization does a good job of reproducing the distribution and strength of the eddy contribution to subduction. Using a spatially-varying coefficient is key to reproduce the regional pattern of the eddy-induced subduction. In addition, the magnitude of the subduction is correctly represented only with a diffusion coefficient that peaks at 104 m2 s−1 in the most energetic areas of the Southern Ocean, a factor of ten larger than commonly used in coarse-resolution climate models. Using a diffusion coefficient that is too small will underestimate the contribution of eddies to the ocean sequestration of heat, salt and carbon. Article in Journal/Newspaper Southern Ocean eCite UTAS (University of Tasmania) Southern Ocean Ocean Modelling 39 1-2 146 153 |
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Open Polar |
collection |
eCite UTAS (University of Tasmania) |
op_collection_id |
ftunivtasecite |
language |
English |
topic |
Earth Sciences Oceanography Physical Oceanography |
spellingShingle |
Earth Sciences Oceanography Physical Oceanography Sallee, J-B Rintoul, SR Parameterization of eddy-induced subduction in the Southern Ocean surface-layer |
topic_facet |
Earth Sciences Oceanography Physical Oceanography |
description |
The divergence of the eddy mass flux in the surface layer of the Southern Ocean makes an important contribution to subduction of fluid through the base of the mixed layer. Therefore, accurate parameterization of this process is needed to correctly represent the Southern Ocean ventilation in coarse-resolution models. We test a common approach to the parameterization of eddy fluxes (Gent and McWilliams, 1990) using output from the 1/6 eddy-permitting Southern Ocean State Estimate, which assimilates a variety of ocean observations using an adjoint method. When a constant diffusion coefficient of conventional magnitude O(1000 m2 s−1) is used, the parameterized fluxes fail to reproduce the regional pattern and magnitude of eddy-driven subduction diagnosed from the model. However, when an appropriate choice is made for the diffusion coefficient, the parameterization does a good job of reproducing the distribution and strength of the eddy contribution to subduction. Using a spatially-varying coefficient is key to reproduce the regional pattern of the eddy-induced subduction. In addition, the magnitude of the subduction is correctly represented only with a diffusion coefficient that peaks at 104 m2 s−1 in the most energetic areas of the Southern Ocean, a factor of ten larger than commonly used in coarse-resolution climate models. Using a diffusion coefficient that is too small will underestimate the contribution of eddies to the ocean sequestration of heat, salt and carbon. |
format |
Article in Journal/Newspaper |
author |
Sallee, J-B Rintoul, SR |
author_facet |
Sallee, J-B Rintoul, SR |
author_sort |
Sallee, J-B |
title |
Parameterization of eddy-induced subduction in the Southern Ocean surface-layer |
title_short |
Parameterization of eddy-induced subduction in the Southern Ocean surface-layer |
title_full |
Parameterization of eddy-induced subduction in the Southern Ocean surface-layer |
title_fullStr |
Parameterization of eddy-induced subduction in the Southern Ocean surface-layer |
title_full_unstemmed |
Parameterization of eddy-induced subduction in the Southern Ocean surface-layer |
title_sort |
parameterization of eddy-induced subduction in the southern ocean surface-layer |
publisher |
Elsevier Sci Ltd |
publishDate |
2011 |
url |
https://doi.org/10.1016/j.ocemod.2011.04.001 http://ecite.utas.edu.au/80635 |
geographic |
Southern Ocean |
geographic_facet |
Southern Ocean |
genre |
Southern Ocean |
genre_facet |
Southern Ocean |
op_relation |
http://dx.doi.org/10.1016/j.ocemod.2011.04.001 Sallee, J-B and Rintoul, SR, Parameterization of eddy-induced subduction in the Southern Ocean surface-layer, Ocean Modelling, 39, (1-2) pp. 146-153. ISSN 1463-5003 (2011) [Refereed Article] http://ecite.utas.edu.au/80635 |
op_doi |
https://doi.org/10.1016/j.ocemod.2011.04.001 |
container_title |
Ocean Modelling |
container_volume |
39 |
container_issue |
1-2 |
container_start_page |
146 |
op_container_end_page |
153 |
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1766204674693660672 |