Modal Decay in the Australia–Antarctic Basin

The barotropic intraseasonal variability in the Australia–Antarctic Basin (AAB) is studied in terms of the excitation and decay of topographically trapped barotropic modes. The main objective is to reconcile two widely differing estimates of the decay rate of sea surface height (SSH) anomalies in th...

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Main Authors: Wilbert Weijer, Sarah T. Gille
Other Authors: The Pennsylvania State University CiteSeerX Archives
Format: Text
Language:English
Published: 2009
Subjects:
Online Access:http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.412.1779
http://www-pord.ucsd.edu/~sgille/pub_dir/i1520-0485-39-11-2893.pdf
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spelling ftciteseerx:oai:CiteSeerX.psu:10.1.1.412.1779 2023-05-15T13:45:34+02:00 Modal Decay in the Australia–Antarctic Basin Wilbert Weijer Sarah T. Gille The Pennsylvania State University CiteSeerX Archives 2009 application/pdf http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.412.1779 http://www-pord.ucsd.edu/~sgille/pub_dir/i1520-0485-39-11-2893.pdf en eng http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.412.1779 http://www-pord.ucsd.edu/~sgille/pub_dir/i1520-0485-39-11-2893.pdf Metadata may be used without restrictions as long as the oai identifier remains attached to it. http://www-pord.ucsd.edu/~sgille/pub_dir/i1520-0485-39-11-2893.pdf text 2009 ftciteseerx 2016-01-08T03:24:00Z The barotropic intraseasonal variability in the Australia–Antarctic Basin (AAB) is studied in terms of the excitation and decay of topographically trapped barotropic modes. The main objective is to reconcile two widely differing estimates of the decay rate of sea surface height (SSH) anomalies in the AAB that are assumed to be related to barotropic modes. First, an empirical orthogonal function (EOF) analysis is applied to almost 15 years of altimeter data. The analysis suggests that several modes are involved in the variability of the AAB, each related to distinct areas with (almost) closed contours of potential vorticity. Second, the dominant normal modes of the AAB are determined in a barotropic shallow-water (SW) model. These stationary modes are confined by the closed contours of potential vorticity that surround the eastern AAB, and the crest of the Southeast Indian Ridge. For reasonable values of horizontal eddy viscosity and bottom friction, their decay time scale is on the order of several weeks. Third, the SW model is forced with realistic winds and integrated for several years. Projection of the modal velocity patterns onto the output fields shows that the barotropic modes are indeed excited in the model, and that they decay slowly on the frictional O(3 weeks) time scale. However, the SSH anomalies in the modal areas display rapid O(4 days) decay. Additional analysis shows that this rapid decay reflects the adjustment of unbalanced flow components through the emission of Rossby waves. Resonant excitation of the dominant free modes accounts for about 20 % of the SSH variability in the forced-model run. Other mechanisms are suggested to explain the region of high SSH variability in the AAB. Text Antarc* Antarctic Unknown Antarctic Indian Southeast Indian Ridge ENVELOPE(110.000,110.000,-50.000,-50.000)
institution Open Polar
collection Unknown
op_collection_id ftciteseerx
language English
description The barotropic intraseasonal variability in the Australia–Antarctic Basin (AAB) is studied in terms of the excitation and decay of topographically trapped barotropic modes. The main objective is to reconcile two widely differing estimates of the decay rate of sea surface height (SSH) anomalies in the AAB that are assumed to be related to barotropic modes. First, an empirical orthogonal function (EOF) analysis is applied to almost 15 years of altimeter data. The analysis suggests that several modes are involved in the variability of the AAB, each related to distinct areas with (almost) closed contours of potential vorticity. Second, the dominant normal modes of the AAB are determined in a barotropic shallow-water (SW) model. These stationary modes are confined by the closed contours of potential vorticity that surround the eastern AAB, and the crest of the Southeast Indian Ridge. For reasonable values of horizontal eddy viscosity and bottom friction, their decay time scale is on the order of several weeks. Third, the SW model is forced with realistic winds and integrated for several years. Projection of the modal velocity patterns onto the output fields shows that the barotropic modes are indeed excited in the model, and that they decay slowly on the frictional O(3 weeks) time scale. However, the SSH anomalies in the modal areas display rapid O(4 days) decay. Additional analysis shows that this rapid decay reflects the adjustment of unbalanced flow components through the emission of Rossby waves. Resonant excitation of the dominant free modes accounts for about 20 % of the SSH variability in the forced-model run. Other mechanisms are suggested to explain the region of high SSH variability in the AAB.
author2 The Pennsylvania State University CiteSeerX Archives
format Text
author Wilbert Weijer
Sarah T. Gille
spellingShingle Wilbert Weijer
Sarah T. Gille
Modal Decay in the Australia–Antarctic Basin
author_facet Wilbert Weijer
Sarah T. Gille
author_sort Wilbert Weijer
title Modal Decay in the Australia–Antarctic Basin
title_short Modal Decay in the Australia–Antarctic Basin
title_full Modal Decay in the Australia–Antarctic Basin
title_fullStr Modal Decay in the Australia–Antarctic Basin
title_full_unstemmed Modal Decay in the Australia–Antarctic Basin
title_sort modal decay in the australia–antarctic basin
publishDate 2009
url http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.412.1779
http://www-pord.ucsd.edu/~sgille/pub_dir/i1520-0485-39-11-2893.pdf
long_lat ENVELOPE(110.000,110.000,-50.000,-50.000)
geographic Antarctic
Indian
Southeast Indian Ridge
geographic_facet Antarctic
Indian
Southeast Indian Ridge
genre Antarc*
Antarctic
genre_facet Antarc*
Antarctic
op_source http://www-pord.ucsd.edu/~sgille/pub_dir/i1520-0485-39-11-2893.pdf
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http://www-pord.ucsd.edu/~sgille/pub_dir/i1520-0485-39-11-2893.pdf
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