Sea Ice Mechanics Research Progress.

The architecture for a new large scale (5 to 100 km, 1 hour to 1 day) sea ice dynamics model based on an anisotropic constitutive law is presented here. This architecture accounts directly for refrozen lead systems in the pack ice strength (with an anisotropic failure surface) and in the ice thickne...

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Main Author: Coon, Max D.
Other Authors: NORTHWEST RESEARCH ASSOCIATES INC BELLEVUE WA
Format: Text
Language:English
Published: 1997
Subjects:
Ice
Online Access:http://www.dtic.mil/docs/citations/ADA327636
http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=ADA327636
id ftdtic:ADA327636
record_format openpolar
spelling ftdtic:ADA327636 2023-05-15T16:37:15+02:00 Sea Ice Mechanics Research Progress. Coon, Max D. NORTHWEST RESEARCH ASSOCIATES INC BELLEVUE WA 1997-07-18 text/html http://www.dtic.mil/docs/citations/ADA327636 http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=ADA327636 en eng http://www.dtic.mil/docs/citations/ADA327636 APPROVED FOR PUBLIC RELEASE DTIC AND NTIS Snow Ice and Permafrost *ICE MECHANICS *SEA ICE SCALE MODELS DEFORMATION FRACTURE(MECHANICS) ANISOTROPY SHEAR STRESSES ELASTOPLASTICITY BUOYS ICE DYNAMICS MODELS Text 1997 ftdtic 2016-02-19T20:35:11Z The architecture for a new large scale (5 to 100 km, 1 hour to 1 day) sea ice dynamics model based on an anisotropic constitutive law is presented here. This architecture accounts directly for refrozen lead systems in the pack ice strength (with an anisotropic failure surface) and in the ice thickness distribution (with an oriented thickness distribution). The lower limit (5 km) of the model resolution is controlled by the fracture spacing of old, thicker ice and the maximum lead width. The upper limit of the model resolution (100 km) is controlled by curvature in the lead directions and variations in the lead width. These in turn are controlled by the variations in internal ice stress due to driving forces (winds and currents), which set the time resolution. This architecture features abrupt changes in the failure surface and the associated flow rule that cannot be averaged over a time step. In addition, the principal stress normal to a new lead must be zero as it opens. This model has sub-scale simulations that allow for the inclusion of phenomena such as ridging, rafting, buckling, and fracture on the behavior of the ice. With this new ice constitutive law, it is possible to directly test the ice failure strength, plastic flow rule, and ice thickness distribution. The data most useful for this testing come from ice stress and position buoys together with SAR deformation data. Some data comparisons have already been made. Text Ice permafrost Sea ice Defense Technical Information Center: DTIC Technical Reports database
institution Open Polar
collection Defense Technical Information Center: DTIC Technical Reports database
op_collection_id ftdtic
language English
topic Snow
Ice and Permafrost
*ICE MECHANICS
*SEA ICE
SCALE MODELS
DEFORMATION
FRACTURE(MECHANICS)
ANISOTROPY
SHEAR STRESSES
ELASTOPLASTICITY
BUOYS
ICE DYNAMICS MODELS
spellingShingle Snow
Ice and Permafrost
*ICE MECHANICS
*SEA ICE
SCALE MODELS
DEFORMATION
FRACTURE(MECHANICS)
ANISOTROPY
SHEAR STRESSES
ELASTOPLASTICITY
BUOYS
ICE DYNAMICS MODELS
Coon, Max D.
Sea Ice Mechanics Research Progress.
topic_facet Snow
Ice and Permafrost
*ICE MECHANICS
*SEA ICE
SCALE MODELS
DEFORMATION
FRACTURE(MECHANICS)
ANISOTROPY
SHEAR STRESSES
ELASTOPLASTICITY
BUOYS
ICE DYNAMICS MODELS
description The architecture for a new large scale (5 to 100 km, 1 hour to 1 day) sea ice dynamics model based on an anisotropic constitutive law is presented here. This architecture accounts directly for refrozen lead systems in the pack ice strength (with an anisotropic failure surface) and in the ice thickness distribution (with an oriented thickness distribution). The lower limit (5 km) of the model resolution is controlled by the fracture spacing of old, thicker ice and the maximum lead width. The upper limit of the model resolution (100 km) is controlled by curvature in the lead directions and variations in the lead width. These in turn are controlled by the variations in internal ice stress due to driving forces (winds and currents), which set the time resolution. This architecture features abrupt changes in the failure surface and the associated flow rule that cannot be averaged over a time step. In addition, the principal stress normal to a new lead must be zero as it opens. This model has sub-scale simulations that allow for the inclusion of phenomena such as ridging, rafting, buckling, and fracture on the behavior of the ice. With this new ice constitutive law, it is possible to directly test the ice failure strength, plastic flow rule, and ice thickness distribution. The data most useful for this testing come from ice stress and position buoys together with SAR deformation data. Some data comparisons have already been made.
author2 NORTHWEST RESEARCH ASSOCIATES INC BELLEVUE WA
format Text
author Coon, Max D.
author_facet Coon, Max D.
author_sort Coon, Max D.
title Sea Ice Mechanics Research Progress.
title_short Sea Ice Mechanics Research Progress.
title_full Sea Ice Mechanics Research Progress.
title_fullStr Sea Ice Mechanics Research Progress.
title_full_unstemmed Sea Ice Mechanics Research Progress.
title_sort sea ice mechanics research progress.
publishDate 1997
url http://www.dtic.mil/docs/citations/ADA327636
http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=ADA327636
genre Ice
permafrost
Sea ice
genre_facet Ice
permafrost
Sea ice
op_source DTIC AND NTIS
op_relation http://www.dtic.mil/docs/citations/ADA327636
op_rights APPROVED FOR PUBLIC RELEASE
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