A model of sea ice formation in leads and polynyas

Cracks in the sea ice cover break the barrier between the ocean and atmosphere, exposing the ocean to the cold atmosphere during the winter. These cracks are known as leads within the continuous sea ice pack and polynyas near land or ice shelves. Sea ice formation starts with frazil ice crystals in...

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Published in:Journal of Physical Oceanography
Main Authors: Heorton, Harold D. B. S., Radia, Nikhil, Feltham, Daniel L.
Format: Article in Journal/Newspaper
Language:unknown
Published: American Meteorological Society 2017
Subjects:
Online Access:https://centaur.reading.ac.uk/71200/
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spelling ftunivreading:oai:centaur.reading.ac.uk:71200 2024-09-15T18:12:05+00:00 A model of sea ice formation in leads and polynyas Heorton, Harold D. B. S. Radia, Nikhil Feltham, Daniel L. 2017-07 https://centaur.reading.ac.uk/71200/ unknown American Meteorological Society Heorton, H. D. B. S. <https://centaur.reading.ac.uk/view/creators/90005743.html>, Radia, N. and Feltham, D. L. <https://centaur.reading.ac.uk/view/creators/90004991.html> orcid:0000-0003-2289-014X (2017) A model of sea ice formation in leads and polynyas. Journal of Physical Oceanography, 47 (7). pp. 1701-1718. ISSN 0022-3670 doi: https://doi.org/10.1175/jpo-d-16-0224.1 <https://doi.org/10.1175/jpo-d-16-0224.1> Article PeerReviewed 2017 ftunivreading https://doi.org/10.1175/jpo-d-16-0224.1 2024-06-25T15:00:51Z Cracks in the sea ice cover break the barrier between the ocean and atmosphere, exposing the ocean to the cold atmosphere during the winter. These cracks are known as leads within the continuous sea ice pack and polynyas near land or ice shelves. Sea ice formation starts with frazil ice crystals in supercooled waters, which grow and precipitate to the ocean surface to form grease ice, eventually consolidating into a layer of solid sea ice that grows downward. In this study, a numerical model is formulated to simulate the formation of sea ice in a lead or polynya from frazil ice to a layer of new sea ice. The simulations show the refreezing of a lead within 48 h of its opening. Grease ice covers the lead typically within 3–10 h and consolidates into sea ice within 15–30 h. This study uses its model to simulate an observed polynya event in the Laptev Sea showing the vertical distribution of frazil ice and water supercooling. Sensitivity studies are used to investigate the dependence of ice growth on the ambient environment with the surface wind speed shown to be of greatest importance to lead exposure time and total ice growth. The size and distribution of frazil crystals and the time taken for the lead to freeze over is shown to be highly dependent upon the ambient forcing and lead geometry. Article in Journal/Newspaper ice pack Ice Shelves laptev Laptev Sea Sea ice CentAUR: Central Archive at the University of Reading Journal of Physical Oceanography 47 7 1701 1718
institution Open Polar
collection CentAUR: Central Archive at the University of Reading
op_collection_id ftunivreading
language unknown
description Cracks in the sea ice cover break the barrier between the ocean and atmosphere, exposing the ocean to the cold atmosphere during the winter. These cracks are known as leads within the continuous sea ice pack and polynyas near land or ice shelves. Sea ice formation starts with frazil ice crystals in supercooled waters, which grow and precipitate to the ocean surface to form grease ice, eventually consolidating into a layer of solid sea ice that grows downward. In this study, a numerical model is formulated to simulate the formation of sea ice in a lead or polynya from frazil ice to a layer of new sea ice. The simulations show the refreezing of a lead within 48 h of its opening. Grease ice covers the lead typically within 3–10 h and consolidates into sea ice within 15–30 h. This study uses its model to simulate an observed polynya event in the Laptev Sea showing the vertical distribution of frazil ice and water supercooling. Sensitivity studies are used to investigate the dependence of ice growth on the ambient environment with the surface wind speed shown to be of greatest importance to lead exposure time and total ice growth. The size and distribution of frazil crystals and the time taken for the lead to freeze over is shown to be highly dependent upon the ambient forcing and lead geometry.
format Article in Journal/Newspaper
author Heorton, Harold D. B. S.
Radia, Nikhil
Feltham, Daniel L.
spellingShingle Heorton, Harold D. B. S.
Radia, Nikhil
Feltham, Daniel L.
A model of sea ice formation in leads and polynyas
author_facet Heorton, Harold D. B. S.
Radia, Nikhil
Feltham, Daniel L.
author_sort Heorton, Harold D. B. S.
title A model of sea ice formation in leads and polynyas
title_short A model of sea ice formation in leads and polynyas
title_full A model of sea ice formation in leads and polynyas
title_fullStr A model of sea ice formation in leads and polynyas
title_full_unstemmed A model of sea ice formation in leads and polynyas
title_sort model of sea ice formation in leads and polynyas
publisher American Meteorological Society
publishDate 2017
url https://centaur.reading.ac.uk/71200/
genre ice pack
Ice Shelves
laptev
Laptev Sea
Sea ice
genre_facet ice pack
Ice Shelves
laptev
Laptev Sea
Sea ice
op_relation Heorton, H. D. B. S. <https://centaur.reading.ac.uk/view/creators/90005743.html>, Radia, N. and Feltham, D. L. <https://centaur.reading.ac.uk/view/creators/90004991.html> orcid:0000-0003-2289-014X (2017) A model of sea ice formation in leads and polynyas. Journal of Physical Oceanography, 47 (7). pp. 1701-1718. ISSN 0022-3670 doi: https://doi.org/10.1175/jpo-d-16-0224.1 <https://doi.org/10.1175/jpo-d-16-0224.1>
op_doi https://doi.org/10.1175/jpo-d-16-0224.1
container_title Journal of Physical Oceanography
container_volume 47
container_issue 7
container_start_page 1701
op_container_end_page 1718
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