Lamont-Doherty Earth Observatory

The sea ice distribution in the Antarctic polar oceans is intimately tied to the underlying ocean structure, which controls the oceans ' vertical heat flux and stability. The former determines the rate at which ice grows for a given air-sea heat flux, while the latter limits the amount of sea i...

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Main Authors: Douglas G. Martinson, Richard A. Iannuzzi
Other Authors: The Pennsylvania State University CiteSeerX Archives
Format: Text
Language:English
Subjects:
Online Access:http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.514.5037
http://www.ldeo.columbia.edu/res/div/ocp/pub/martinson/Martinson_and_Iannuzzi_1998.pdf
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spelling ftciteseerx:oai:CiteSeerX.psu:10.1.1.514.5037 2023-05-15T13:57:06+02:00 Lamont-Doherty Earth Observatory Douglas G. Martinson Richard A. Iannuzzi The Pennsylvania State University CiteSeerX Archives application/pdf http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.514.5037 http://www.ldeo.columbia.edu/res/div/ocp/pub/martinson/Martinson_and_Iannuzzi_1998.pdf en eng http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.514.5037 http://www.ldeo.columbia.edu/res/div/ocp/pub/martinson/Martinson_and_Iannuzzi_1998.pdf Metadata may be used without restrictions as long as the oai identifier remains attached to it. http://www.ldeo.columbia.edu/res/div/ocp/pub/martinson/Martinson_and_Iannuzzi_1998.pdf text ftciteseerx 2016-01-08T09:48:29Z The sea ice distribution in the Antarctic polar oceans is intimately tied to the underlying ocean structure, which controls the oceans ' vertical heat flux and stability. The former determines the rate at which ice grows for a given air-sea heat flux, while the latter limits the amount of sea ice that can grow locally before overturning the water column. These relationships have been described through a set of scalings, allowing us to estimate, through examination of the vertical distributions of ocean temperature and salinity: (1) the maximum amount of in situ ice growth in any one location, (2) the ratio of ice melt to ice growth, (3) the amount of ice that has melted in any particular summer location, (4) the ocean winter-averaged heat flux. Climatological maps of these quantities are presented for the Weddell gyre region and general results described. Results include: (1) the sea ice cover throughout the seasonal sea ice region is typically 0.6 m thick or less by the spring melt period, though it is thinner than 0.3 m in some regions near the gyre core; (2) the ocean-ice system manages to liberate heat from the deep water at an average winter rate of 25-35 W/m2 throughout the gyre, regardless of the large scale stratification and dynamic setting which reflect different processes by which the heat makes its way to the surface from the deep waters; (3) Text Antarc* Antarctic Sea ice Unknown Antarctic The Antarctic Weddell
institution Open Polar
collection Unknown
op_collection_id ftciteseerx
language English
description The sea ice distribution in the Antarctic polar oceans is intimately tied to the underlying ocean structure, which controls the oceans ' vertical heat flux and stability. The former determines the rate at which ice grows for a given air-sea heat flux, while the latter limits the amount of sea ice that can grow locally before overturning the water column. These relationships have been described through a set of scalings, allowing us to estimate, through examination of the vertical distributions of ocean temperature and salinity: (1) the maximum amount of in situ ice growth in any one location, (2) the ratio of ice melt to ice growth, (3) the amount of ice that has melted in any particular summer location, (4) the ocean winter-averaged heat flux. Climatological maps of these quantities are presented for the Weddell gyre region and general results described. Results include: (1) the sea ice cover throughout the seasonal sea ice region is typically 0.6 m thick or less by the spring melt period, though it is thinner than 0.3 m in some regions near the gyre core; (2) the ocean-ice system manages to liberate heat from the deep water at an average winter rate of 25-35 W/m2 throughout the gyre, regardless of the large scale stratification and dynamic setting which reflect different processes by which the heat makes its way to the surface from the deep waters; (3)
author2 The Pennsylvania State University CiteSeerX Archives
format Text
author Douglas G. Martinson
Richard A. Iannuzzi
spellingShingle Douglas G. Martinson
Richard A. Iannuzzi
Lamont-Doherty Earth Observatory
author_facet Douglas G. Martinson
Richard A. Iannuzzi
author_sort Douglas G. Martinson
title Lamont-Doherty Earth Observatory
title_short Lamont-Doherty Earth Observatory
title_full Lamont-Doherty Earth Observatory
title_fullStr Lamont-Doherty Earth Observatory
title_full_unstemmed Lamont-Doherty Earth Observatory
title_sort lamont-doherty earth observatory
url http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.514.5037
http://www.ldeo.columbia.edu/res/div/ocp/pub/martinson/Martinson_and_Iannuzzi_1998.pdf
geographic Antarctic
The Antarctic
Weddell
geographic_facet Antarctic
The Antarctic
Weddell
genre Antarc*
Antarctic
Sea ice
genre_facet Antarc*
Antarctic
Sea ice
op_source http://www.ldeo.columbia.edu/res/div/ocp/pub/martinson/Martinson_and_Iannuzzi_1998.pdf
op_relation http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.514.5037
http://www.ldeo.columbia.edu/res/div/ocp/pub/martinson/Martinson_and_Iannuzzi_1998.pdf
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