Two Configurations of the Western Arctic Shelfbreak Current in Summer

Data from a closely spaced array of moorings situated across the Beaufort Sea shelfbreak at 152°W are used to study the Western Arctic Shelfbreak Current, with emphasis on its configuration during the summer season. Two dynamically distinct states of the current are revealed in the absence of wind,...

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Bibliographic Details
Main Authors: Von Appen, Wilken-Jon (Contributor), Pickart, Robert S. (Author)
Other Authors: Massachusetts Institute of Technology. Department of Earth, Atmospheric, and Planetary Sciences (Contributor)
Format: Article
Language:English
Published: American Meteorological Society, 2012-10-25T17:59:57Z.
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Online Access:Get fulltext
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100 1 0 |a Von Appen, Wilken-Jon  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Earth, Atmospheric, and Planetary Sciences  |e contributor 
100 1 0 |a Von Appen, Wilken-Jon  |e contributor 
700 1 0 |a Pickart, Robert S.  |e author 
245 0 0 |a Two Configurations of the Western Arctic Shelfbreak Current in Summer 
260 |b American Meteorological Society,   |c 2012-10-25T17:59:57Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/74253 
520 |a Data from a closely spaced array of moorings situated across the Beaufort Sea shelfbreak at 152°W are used to study the Western Arctic Shelfbreak Current, with emphasis on its configuration during the summer season. Two dynamically distinct states of the current are revealed in the absence of wind, with each lasting approximately one month. The first is a surface-intensified shelfbreak jet transporting warm and buoyant Alaskan Coastal Water in late summer. This is the eastward continuation of the Alaskan Coastal Current. It is both baroclinically and barotropically unstable and hence capable of forming the surface-intensified warm-core eddies observed in the southern Beaufort Sea. The second configuration, present during early summer, is a bottom-intensified shelfbreak current advecting weakly stratified Chukchi Summer Water. It is baroclinically unstable and likely forms the middepth warm-core eddies present in the interior basin. The mesoscale instabilities extract energy from the mean flow such that the surface-intensified jet should spin down over an e-folding distance of 300 km beyond the array site, whereas the bottom-intensified configuration should decay within 150 km. This implies that Pacific Summer Water does not extend far into the Canadian Beaufort Sea as a well-defined shelfbreak current. In contrast, the Pacific Winter Water configuration of the shelfbreak jet is estimated to decay over a much greater distance of approximately 1400 km, implying that it should reach the first entrance to the Canadian Arctic Archipelago. 
520 |a National Science Foundation (U.S.) (Grant OCE-0726640) 
520 |a National Science Foundation (U.S.) (Grant OPP-0731928) 
520 |a National Science Foundation (U.S.) (Grant OPP-0713250) 
546 |a en_US 
655 7 |a Article 
773 |t Journal of Physical Oceanography