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...
Published in: | Journal of Physical Oceanography |
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American Meteorological Society
2017
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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 |
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CentAUR: Central Archive at the University of Reading |
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ftunivreading |
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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 |
_version_ |
1810449678662107136 |