Modelling the rheology of sea ice as a collection of diamond-shaped floes

In polar oceans, seawater freezes to form a layer of sea ice of several metres thickness that can cover up to 8% of the Earth's surface. The modelled sea ice cover state is described by thickness and orientational distribution of interlocking, anisotropic diamond-shaped ice floes delineated by...

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Main Authors: Wilchinsky, AV, Feltham, DL
Format: Article in Journal/Newspaper
Language:unknown
Published: ELSEVIER SCIENCE BV 2006
Subjects:
Online Access:http://discovery.ucl.ac.uk/154806/
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spelling ftucl:oai:eprints.ucl.ac.uk.OAI2:154806 2023-05-15T18:16:25+02:00 Modelling the rheology of sea ice as a collection of diamond-shaped floes Wilchinsky, AV Feltham, DL 2006-09-30 http://discovery.ucl.ac.uk/154806/ unknown ELSEVIER SCIENCE BV J NON-NEWTON FLUID , 138 (1) 22 - 32. (2006) sea ice stress anisotropy ANISOTROPIC MODEL PACK ICE DYNAMICS Article 2006 ftucl 2016-11-17T23:16:12Z In polar oceans, seawater freezes to form a layer of sea ice of several metres thickness that can cover up to 8% of the Earth's surface. The modelled sea ice cover state is described by thickness and orientational distribution of interlocking, anisotropic diamond-shaped ice floes delineated by slip lines, as supported by observation. The purpose of this study is to develop a set of equations describing the mean-field sea ice stresses that result from interactions between the ice floes and the evolution of the ice floe orientation, which are simple enough to be incorporated into a climate model. The sea ice stress caused by a deformation of the ice cover is determined by employing an existing kinematic model of ice floe motion, which enables us to calculate the forces acting on the ice floes due to crushing into and sliding past each other, and then by averaging over all possible floe orientations. We describe the orientational floe distribution with a structure tensor and propose an evolution equation for this tensor that accounts for rigid body rotation of the floes, their apparent re-orientation due to new slip line formation, and change of shape of the floes due to freezing and melting. The form of the evolution equation proposed is motivated by laboratory observations of sea ice failure under controlled conditions. Finally, we present simulations of the evolution of sea ice stress and floe orientation for several imposed flow types. Although evidence to test the simulations against is lacking, the simulations seem physically reasonable. (c) 2006 Elsevier B.V. All rights reserved. Article in Journal/Newspaper Sea ice University College London: UCL Discovery
institution Open Polar
collection University College London: UCL Discovery
op_collection_id ftucl
language unknown
topic sea ice
stress
anisotropy
ANISOTROPIC MODEL
PACK ICE
DYNAMICS
spellingShingle sea ice
stress
anisotropy
ANISOTROPIC MODEL
PACK ICE
DYNAMICS
Wilchinsky, AV
Feltham, DL
Modelling the rheology of sea ice as a collection of diamond-shaped floes
topic_facet sea ice
stress
anisotropy
ANISOTROPIC MODEL
PACK ICE
DYNAMICS
description In polar oceans, seawater freezes to form a layer of sea ice of several metres thickness that can cover up to 8% of the Earth's surface. The modelled sea ice cover state is described by thickness and orientational distribution of interlocking, anisotropic diamond-shaped ice floes delineated by slip lines, as supported by observation. The purpose of this study is to develop a set of equations describing the mean-field sea ice stresses that result from interactions between the ice floes and the evolution of the ice floe orientation, which are simple enough to be incorporated into a climate model. The sea ice stress caused by a deformation of the ice cover is determined by employing an existing kinematic model of ice floe motion, which enables us to calculate the forces acting on the ice floes due to crushing into and sliding past each other, and then by averaging over all possible floe orientations. We describe the orientational floe distribution with a structure tensor and propose an evolution equation for this tensor that accounts for rigid body rotation of the floes, their apparent re-orientation due to new slip line formation, and change of shape of the floes due to freezing and melting. The form of the evolution equation proposed is motivated by laboratory observations of sea ice failure under controlled conditions. Finally, we present simulations of the evolution of sea ice stress and floe orientation for several imposed flow types. Although evidence to test the simulations against is lacking, the simulations seem physically reasonable. (c) 2006 Elsevier B.V. All rights reserved.
format Article in Journal/Newspaper
author Wilchinsky, AV
Feltham, DL
author_facet Wilchinsky, AV
Feltham, DL
author_sort Wilchinsky, AV
title Modelling the rheology of sea ice as a collection of diamond-shaped floes
title_short Modelling the rheology of sea ice as a collection of diamond-shaped floes
title_full Modelling the rheology of sea ice as a collection of diamond-shaped floes
title_fullStr Modelling the rheology of sea ice as a collection of diamond-shaped floes
title_full_unstemmed Modelling the rheology of sea ice as a collection of diamond-shaped floes
title_sort modelling the rheology of sea ice as a collection of diamond-shaped floes
publisher ELSEVIER SCIENCE BV
publishDate 2006
url http://discovery.ucl.ac.uk/154806/
genre Sea ice
genre_facet Sea ice
op_source J NON-NEWTON FLUID , 138 (1) 22 - 32. (2006)
_version_ 1766190027046387712