Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model

The eddy-induced mass transport is diagnosed for the Southern Ocean in an eddy-permitting global ocean model (OCCAM). The focus is on the transport by transient eddies in the deep ocean. The transport streamfunction is calculated in four different combinations of coordinate system. Depending on the...

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Published in:Ocean Modelling
Main Authors: Lee, M-M., Coward, A.
Format: Article in Journal/Newspaper
Language:unknown
Published: 2003
Subjects:
Online Access:http://nora.nerc.ac.uk/id/eprint/102049/
https://doi.org/10.1016/S1463-5003(02)00044-6
id ftnerc:oai:nora.nerc.ac.uk:102049
record_format openpolar
spelling ftnerc:oai:nora.nerc.ac.uk:102049 2023-05-15T13:45:12+02:00 Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model Lee, M-M. Coward, A. 2003 http://nora.nerc.ac.uk/id/eprint/102049/ https://doi.org/10.1016/S1463-5003(02)00044-6 unknown Lee, M-M.; Coward, A. orcid:0000-0002-9111-7700 . 2003 Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model. Ocean Modelling, 5 (3). 249-266. https://doi.org/10.1016/S1463-5003(02)00044-6 <https://doi.org/10.1016/S1463-5003(02)00044-6> Publication - Article PeerReviewed 2003 ftnerc https://doi.org/10.1016/S1463-5003(02)00044-6 2023-02-04T19:33:33Z The eddy-induced mass transport is diagnosed for the Southern Ocean in an eddy-permitting global ocean model (OCCAM). The focus is on the transport by transient eddies in the deep ocean. The transport streamfunction is calculated in four different combinations of coordinate system. Depending on the coordinate system employed, the strength of transient eddy transport varies from 6 Sv meridional transport in latitude-density coordinates to 20 Sv across-streamline transport in streamline-depth coordinates. It is shown that transient eddies as well as standing eddies are necessary for cancelling the Deacon cell. In the Antarctic bottom water density layer, the major contribution of the transient eddies towards net equatorward transport occurs (a) as a strong transport over the narrow Drake Passage and (b) as a weaker but systematic transport over a broader region in the southeast Pacific where the Antarctic circumpolar current breaks up into multiple jets. In contrast, in the North Atlantic deep water density layer the net poleward eddy transport is spread out almost everywhere. This suggests that attention to eddies should not be restricted to places where the eddy transport has large magnitude. Article in Journal/Newspaper Antarc* Antarctic Drake Passage North Atlantic Deep Water North Atlantic Southern Ocean Natural Environment Research Council: NERC Open Research Archive Antarctic Southern Ocean The Antarctic Drake Passage Pacific Deacon ENVELOPE(-59.987,-59.987,-73.248,-73.248) Ocean Modelling 5 3 249 266
institution Open Polar
collection Natural Environment Research Council: NERC Open Research Archive
op_collection_id ftnerc
language unknown
description The eddy-induced mass transport is diagnosed for the Southern Ocean in an eddy-permitting global ocean model (OCCAM). The focus is on the transport by transient eddies in the deep ocean. The transport streamfunction is calculated in four different combinations of coordinate system. Depending on the coordinate system employed, the strength of transient eddy transport varies from 6 Sv meridional transport in latitude-density coordinates to 20 Sv across-streamline transport in streamline-depth coordinates. It is shown that transient eddies as well as standing eddies are necessary for cancelling the Deacon cell. In the Antarctic bottom water density layer, the major contribution of the transient eddies towards net equatorward transport occurs (a) as a strong transport over the narrow Drake Passage and (b) as a weaker but systematic transport over a broader region in the southeast Pacific where the Antarctic circumpolar current breaks up into multiple jets. In contrast, in the North Atlantic deep water density layer the net poleward eddy transport is spread out almost everywhere. This suggests that attention to eddies should not be restricted to places where the eddy transport has large magnitude.
format Article in Journal/Newspaper
author Lee, M-M.
Coward, A.
spellingShingle Lee, M-M.
Coward, A.
Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model
author_facet Lee, M-M.
Coward, A.
author_sort Lee, M-M.
title Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model
title_short Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model
title_full Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model
title_fullStr Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model
title_full_unstemmed Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model
title_sort eddy mass transport for the southern ocean in an eddy-permitting global ocean model
publishDate 2003
url http://nora.nerc.ac.uk/id/eprint/102049/
https://doi.org/10.1016/S1463-5003(02)00044-6
long_lat ENVELOPE(-59.987,-59.987,-73.248,-73.248)
geographic Antarctic
Southern Ocean
The Antarctic
Drake Passage
Pacific
Deacon
geographic_facet Antarctic
Southern Ocean
The Antarctic
Drake Passage
Pacific
Deacon
genre Antarc*
Antarctic
Drake Passage
North Atlantic Deep Water
North Atlantic
Southern Ocean
genre_facet Antarc*
Antarctic
Drake Passage
North Atlantic Deep Water
North Atlantic
Southern Ocean
op_relation Lee, M-M.; Coward, A. orcid:0000-0002-9111-7700 . 2003 Eddy mass transport for the Southern Ocean in an eddy-permitting global ocean model. Ocean Modelling, 5 (3). 249-266. https://doi.org/10.1016/S1463-5003(02)00044-6 <https://doi.org/10.1016/S1463-5003(02)00044-6>
op_doi https://doi.org/10.1016/S1463-5003(02)00044-6
container_title Ocean Modelling
container_volume 5
container_issue 3
container_start_page 249
op_container_end_page 266
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