Frazil ice formation in ice shelf water plume

We present a model for the growth of frazil ice crystals and their accumulation as marine ice at the base of Antarctic ice shelves. The model describes the flow of buoyant water upward along the ice shelf base and includes the differential growth of a range of crystal sizes. Frazil ice formation sta...

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Published in:Journal of Geophysical Research: Oceans
Main Authors: Smedsrud, Lars Henrik, Jenkins, Adrian
Format: Article in Journal/Newspaper
Language:English
Published: American Geophysical Union 2004
Subjects:
Online Access:https://hdl.handle.net/1956/614
https://doi.org/10.1029/2003jc001851
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spelling ftunivbergen:oai:bora.uib.no:1956/614 2023-05-15T13:39:45+02:00 Frazil ice formation in ice shelf water plume Smedsrud, Lars Henrik Jenkins, Adrian 2004-03-17 6495261 bytes application/pdf https://hdl.handle.net/1956/614 https://doi.org/10.1029/2003jc001851 eng eng American Geophysical Union urn:issn:0148-0227 https://hdl.handle.net/1956/614 https://doi.org/10.1029/2003jc001851 Journal article 2004 ftunivbergen https://doi.org/10.1029/2003jc001851 2023-03-14T17:41:26Z We present a model for the growth of frazil ice crystals and their accumulation as marine ice at the base of Antarctic ice shelves. The model describes the flow of buoyant water upward along the ice shelf base and includes the differential growth of a range of crystal sizes. Frazil ice formation starts when the rising plume becomes supercooled. Initially, the majority of crystals have a radius of ∼0.3 mm and concentrations are below 0.1 g/L. Depending on the ice shelf slope, which controls the plume speed, frazil crystals increase in size and number. Typically, crystals up to 1.0 mm in radius are kept in suspension, and concentrations reach a maximum of 0.4 g/L. The frazil ice in suspension decreases the plume density and thus increases the plume speed. Larger crystals precipitate upward onto the ice shelf base first, with smaller crystals following as the plume slows down. In this way, marine ice is formed at rates of up to 4 m/yr in some places, consistent with areas of observed basal accumulation on Filchner-Ronne Ice Shelf. The plume continues below the ice shelf as long as it is buoyant. If the plume reaches the ice front, its rapid rise produces high supercooling and the ice crystals attain a radius of several millimeters before reaching the surface. Similar ice crystals have been trawled at depth north of Antarctic ice shelves, but otherwise no observations exist to verify these first predictions of ice crystal sizes and volumes. Article in Journal/Newspaper Antarc* Antarctic Filchner Ronne Ice Shelf Filchner-Ronne Ice Shelf Ice Shelf Ice Shelves Ronne Ice Shelf University of Bergen: Bergen Open Research Archive (BORA-UiB) Antarctic Ronne Ice Shelf ENVELOPE(-61.000,-61.000,-78.500,-78.500) Journal of Geophysical Research: Oceans 109 C3
institution Open Polar
collection University of Bergen: Bergen Open Research Archive (BORA-UiB)
op_collection_id ftunivbergen
language English
description We present a model for the growth of frazil ice crystals and their accumulation as marine ice at the base of Antarctic ice shelves. The model describes the flow of buoyant water upward along the ice shelf base and includes the differential growth of a range of crystal sizes. Frazil ice formation starts when the rising plume becomes supercooled. Initially, the majority of crystals have a radius of ∼0.3 mm and concentrations are below 0.1 g/L. Depending on the ice shelf slope, which controls the plume speed, frazil crystals increase in size and number. Typically, crystals up to 1.0 mm in radius are kept in suspension, and concentrations reach a maximum of 0.4 g/L. The frazil ice in suspension decreases the plume density and thus increases the plume speed. Larger crystals precipitate upward onto the ice shelf base first, with smaller crystals following as the plume slows down. In this way, marine ice is formed at rates of up to 4 m/yr in some places, consistent with areas of observed basal accumulation on Filchner-Ronne Ice Shelf. The plume continues below the ice shelf as long as it is buoyant. If the plume reaches the ice front, its rapid rise produces high supercooling and the ice crystals attain a radius of several millimeters before reaching the surface. Similar ice crystals have been trawled at depth north of Antarctic ice shelves, but otherwise no observations exist to verify these first predictions of ice crystal sizes and volumes.
format Article in Journal/Newspaper
author Smedsrud, Lars Henrik
Jenkins, Adrian
spellingShingle Smedsrud, Lars Henrik
Jenkins, Adrian
Frazil ice formation in ice shelf water plume
author_facet Smedsrud, Lars Henrik
Jenkins, Adrian
author_sort Smedsrud, Lars Henrik
title Frazil ice formation in ice shelf water plume
title_short Frazil ice formation in ice shelf water plume
title_full Frazil ice formation in ice shelf water plume
title_fullStr Frazil ice formation in ice shelf water plume
title_full_unstemmed Frazil ice formation in ice shelf water plume
title_sort frazil ice formation in ice shelf water plume
publisher American Geophysical Union
publishDate 2004
url https://hdl.handle.net/1956/614
https://doi.org/10.1029/2003jc001851
long_lat ENVELOPE(-61.000,-61.000,-78.500,-78.500)
geographic Antarctic
Ronne Ice Shelf
geographic_facet Antarctic
Ronne Ice Shelf
genre Antarc*
Antarctic
Filchner Ronne Ice Shelf
Filchner-Ronne Ice Shelf
Ice Shelf
Ice Shelves
Ronne Ice Shelf
genre_facet Antarc*
Antarctic
Filchner Ronne Ice Shelf
Filchner-Ronne Ice Shelf
Ice Shelf
Ice Shelves
Ronne Ice Shelf
op_relation urn:issn:0148-0227
https://hdl.handle.net/1956/614
https://doi.org/10.1029/2003jc001851
op_doi https://doi.org/10.1029/2003jc001851
container_title Journal of Geophysical Research: Oceans
container_volume 109
container_issue C3
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