Structure of Boundary Current in the Nansen Basin of the Arctic Ocean
Andrey V. Pnyushkov1, Igor V. Polyakov2, Vladimir V. Ivanov3
1International Arctic Research Center, University of Alaska Fairbanks, 930 Koyukuk Drive , Fairbanks, AK, 99775, USA, Phone 907-474-2683, andrey [at] iarc [dot] uaf [dot] edu
2International Arctic Research Center, University of Alaska Fairbanks, 930 Koyukuk Drive , Fairbanks, AK, 99775, USA, Phone 907-474-2686, igor [at] iarc [dot] uaf [dot] edu
3Arctic and Antarctic Research Institute, Bering Street, 38, St. Petersburg, 199397, Russia, Phone +7-812-352-3352, vladimir [dot] ivanov [at] aari [dot] ru
It is believed that circulation of the intermediate (150-800m) water of Atlantic origin (the so-called Atlantic Water, AW) in the eastern Arctic Ocean is topography-steered confining with deep-basin margins and enveloping the shelf breaks. However, recent observations from Fram Strait show barotropic structure of water transport. Mooring records from Svalbard area (~30E) show very different structure of flow with a maximum velocity at ~200m in the AW core. Mooring observations over the Laptev slope showed erosion of the AW jet-like flow and further eastward observations at the Lomonosov Ridge found a barotropic flow with velocity generally decreasing with depth. Modeling results suggest the existence of topographically-controlled two-core along-slope flow near the Spitsbergen slope. The shallow core is located over the shelf break at ~400m. The second core is shifted in the basin interior and located at ~1200m. Similar to observations, the vertical structure of deeper branch of AW flow has a maximum at an intermediate depth caused by baroclinic balance of forces. This finding may be important for interpretation of warm AW pulses in the Arctic Ocean interior.