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  5. <title>UTas ePrints - Ocean response and feedback to the SST dipole in the Tropical Atlantic</title>
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  13. <meta content="Joyce, T.M." name="eprints.creators_name" />
  14. <meta content="Frankignoul, C." name="eprints.creators_name" />
  15. <meta content="Yang, J." name="eprints.creators_name" />
  16. <meta content="Phillips, Helen E." name="eprints.creators_name" />
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  25. <meta content="Ocean response and feedback to the SST dipole in the Tropical Atlantic" name="eprints.title" />
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  27. <meta content="260403" name="eprints.subjects" />
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  29. <meta content="Atlantic, SST, dipole, feedback, climate, equatorial" name="eprints.keywords" />
  30. <meta content="The equatorial SST dipole represents a mode of climate variability in the tropical Atlantic Ocean that is
  31. closely tied to cross-equatorial flow in the atmosphere, from the cold to the warm hemisphere. It has been
  32. suggested that this mode is sustained by a positive feedback of the tropical winds on the cross-equatorial SST
  33. gradient. The role, if any, of the tropical ocean is the focus of this investigation, which shows that at the latitudes
  34. of the SST signal (centered on 108N/S) there is a weak positive feedback suggested in data from the last half
  35. century, that the cross-equatorial wind stress is closely coupled to this SST gradient on monthly time scales
  36. with no discernable lag, and that the period from January to June is the most active period for coupling. Northward
  37. (southward) anomalies of cross-equatorial wind stress are associated with a substantial negative (positive) wind
  38. stress curl. This wind system can thus drive a cross-equatorial Sverdrup transport in the ocean from the warm
  39. to the cold side of the equator (opposite the winds) with a temporal lag of only a few months. The oceanic
  40. observations of subsurface temperature and a numerical model hindcast also indicate a clear relationship between
  41. this mode of wind-driven variability and changes in the zonal transport of the North Equatorial Countercurrent.
  42. It is estimated that the time-dependent oceanic flow is capable of providing a significant contribution to the
  43. damping of the SST dipole but that external forcing is essential to sustaining the coupled variability." name="eprints.abstract" />
  44. <meta content="2004-11" name="eprints.date" />
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  46. <meta content="Journal of Physical Oceanography" name="eprints.publication" />
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  201. 55, 494-501." name="eprints.referencetext" />
  202. <meta content="Joyce, T.M. and Frankignoul, C. and Yang, J. and Phillips, Helen E. (2004) Ocean response and feedback to the SST dipole in the Tropical Atlantic. Journal of Physical Oceanography, 34 (11). pp. 2525-2540. ISSN 1520-0485" name="eprints.citation" />
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  205. <meta content="Ocean response and feedback to the SST dipole in the Tropical Atlantic" name="DC.title" />
  206. <meta content="Joyce, T.M." name="DC.creator" />
  207. <meta content="Frankignoul, C." name="DC.creator" />
  208. <meta content="Yang, J." name="DC.creator" />
  209. <meta content="Phillips, Helen E." name="DC.creator" />
  210. <meta content="260403 Physical Oceanography" name="DC.subject" />
  211. <meta content="The equatorial SST dipole represents a mode of climate variability in the tropical Atlantic Ocean that is
  212. closely tied to cross-equatorial flow in the atmosphere, from the cold to the warm hemisphere. It has been
  213. suggested that this mode is sustained by a positive feedback of the tropical winds on the cross-equatorial SST
  214. gradient. The role, if any, of the tropical ocean is the focus of this investigation, which shows that at the latitudes
  215. of the SST signal (centered on 108N/S) there is a weak positive feedback suggested in data from the last half
  216. century, that the cross-equatorial wind stress is closely coupled to this SST gradient on monthly time scales
  217. with no discernable lag, and that the period from January to June is the most active period for coupling. Northward
  218. (southward) anomalies of cross-equatorial wind stress are associated with a substantial negative (positive) wind
  219. stress curl. This wind system can thus drive a cross-equatorial Sverdrup transport in the ocean from the warm
  220. to the cold side of the equator (opposite the winds) with a temporal lag of only a few months. The oceanic
  221. observations of subsurface temperature and a numerical model hindcast also indicate a clear relationship between
  222. this mode of wind-driven variability and changes in the zonal transport of the North Equatorial Countercurrent.
  223. It is estimated that the time-dependent oceanic flow is capable of providing a significant contribution to the
  224. damping of the SST dipole but that external forcing is essential to sustaining the coupled variability." name="DC.description" />
  225. <meta content="2004-11" name="DC.date" />
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  336. <h1 class="ep_tm_pagetitle">Ocean response and feedback to the SST dipole in the Tropical Atlantic</h1>
  337. <p style="margin-bottom: 1em" class="not_ep_block"><span class="person_name">Joyce, T.M.</span> and <span class="person_name">Frankignoul, C.</span> and <span class="person_name">Yang, J.</span> and <span class="person_name">Phillips, Helen E.</span> (2004) <xhtml:em>Ocean response and feedback to the SST dipole in the Tropical Atlantic.</xhtml:em> Journal of Physical Oceanography, 34 (11). pp. 2525-2540. ISSN 1520-0485</p><p style="margin-bottom: 1em" class="not_ep_block"></p><table style="margin-bottom: 1em" class="not_ep_block"><tr><td valign="top" style="text-align:center"><a href="http://eprints.utas.edu.au/813/1/Joyce2004jpo.pdf"><img alt="[img]" src="http://eprints.utas.edu.au/style/images/fileicons/application_pdf.png" class="ep_doc_icon" border="0" /></a></td><td valign="top"><a href="http://eprints.utas.edu.au/813/1/Joyce2004jpo.pdf"><span class="ep_document_citation">PDF</span></a> - Full text restricted - Requires a PDF viewer<br />1457Kb</td><td><form method="get" accept-charset="utf-8" action="http://eprints.utas.edu.au/cgi/request_doc"><input accept-charset="utf-8" value="809" name="docid" type="hidden" /><div class=""><input value="Request a copy" name="_action_null" class="ep_form_action_button" onclick="return EPJS_button_pushed( '_action_null' )" type="submit" /> </div></form></td></tr></table><p style="margin-bottom: 1em" class="not_ep_block">Official URL: <a href="http://dx.doi.org/10.1175/JPO2640.1">http://dx.doi.org/10.1175/JPO2640.1</a></p><div class="not_ep_block"><h2>Abstract</h2><p style="padding-bottom: 16px; text-align: left; margin: 1em auto 0em auto">The equatorial SST dipole represents a mode of climate variability in the tropical Atlantic Ocean that is&#13;
  338. closely tied to cross-equatorial flow in the atmosphere, from the cold to the warm hemisphere. It has been&#13;
  339. suggested that this mode is sustained by a positive feedback of the tropical winds on the cross-equatorial SST&#13;
  340. gradient. The role, if any, of the tropical ocean is the focus of this investigation, which shows that at the latitudes&#13;
  341. of the SST signal (centered on 108N/S) there is a weak positive feedback suggested in data from the last half&#13;
  342. century, that the cross-equatorial wind stress is closely coupled to this SST gradient on monthly time scales&#13;
  343. with no discernable lag, and that the period from January to June is the most active period for coupling. Northward&#13;
  344. (southward) anomalies of cross-equatorial wind stress are associated with a substantial negative (positive) wind&#13;
  345. stress curl. This wind system can thus drive a cross-equatorial Sverdrup transport in the ocean from the warm&#13;
  346. to the cold side of the equator (opposite the winds) with a temporal lag of only a few months. The oceanic&#13;
  347. observations of subsurface temperature and a numerical model hindcast also indicate a clear relationship between&#13;
  348. this mode of wind-driven variability and changes in the zonal transport of the North Equatorial Countercurrent.&#13;
  349. It is estimated that the time-dependent oceanic flow is capable of providing a significant contribution to the&#13;
  350. damping of the SST dipole but that external forcing is essential to sustaining the coupled variability.</p></div><table style="margin-bottom: 1em" cellpadding="3" class="not_ep_block" border="0"><tr><th valign="top" class="ep_row">Item Type:</th><td valign="top" class="ep_row">Article</td></tr><tr><th valign="top" class="ep_row">Keywords:</th><td valign="top" class="ep_row">Atlantic, SST, dipole, feedback, climate, equatorial</td></tr><tr><th valign="top" class="ep_row">Subjects:</th><td valign="top" class="ep_row"><a href="http://eprints.utas.edu.au/view/subjects/260403.html">260000 Earth Sciences &gt; 260400 Oceanography &gt; 260403 Physical Oceanography</a></td></tr><tr><th valign="top" class="ep_row">Collections:</th><td valign="top" class="ep_row">UNSPECIFIED</td></tr><tr><th valign="top" class="ep_row">ID Code:</th><td valign="top" class="ep_row">813</td></tr><tr><th valign="top" class="ep_row">Deposited By:</th><td valign="top" class="ep_row"><span class="ep_name_citation"><span class="person_name">Dr Helen E Phillips</span></span></td></tr><tr><th valign="top" class="ep_row">Deposited On:</th><td valign="top" class="ep_row">15 Mar 2007</td></tr><tr><th valign="top" class="ep_row">Last Modified:</th><td valign="top" class="ep_row">08 Feb 2008 12:19</td></tr><tr><th valign="top" class="ep_row">ePrint Statistics:</th><td valign="top" class="ep_row"><a target="ePrintStats" href="/es/index.php?action=show_detail_eprint;id=813;">View statistics for this ePrint</a></td></tr></table><p align="right">Repository Staff Only: <a href="http://eprints.utas.edu.au/cgi/users/home?screen=EPrint::View&amp;eprintid=813">item control page</a></p>
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