Modelling the reorientation of sea-ice faults as the wind changes direction

A discrete-element model of sea ice is used to study how a 90° change in wind direction alters the pattern of faults generated through mechanical failure of the ice. The sea-ice domain is 400km in size and consists of polygonal floes obtained through a Voronoi tessellation. Initially the floes are f...

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Main Authors: Wilchinsky, A. V., Feltham, D. L., Hopkins, M. A.
Format: Article in Journal/Newspaper
Language:English
Published: International Glaciological Society 2011
Subjects:
Online Access:https://centaur.reading.ac.uk/34582/
https://centaur.reading.ac.uk/34582/1/Wilchinsky_etal_2011b.pdf
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spelling ftunivreading:oai:centaur.reading.ac.uk:34582 2024-05-12T07:53:06+00:00 Modelling the reorientation of sea-ice faults as the wind changes direction Wilchinsky, A. V. Feltham, D. L. Hopkins, M. A. 2011 text https://centaur.reading.ac.uk/34582/ https://centaur.reading.ac.uk/34582/1/Wilchinsky_etal_2011b.pdf en eng International Glaciological Society https://centaur.reading.ac.uk/34582/1/Wilchinsky_etal_2011b.pdf Wilchinsky, A. V., Feltham, D. L. <https://centaur.reading.ac.uk/view/creators/90004991.html> and Hopkins, M. A. (2011) Modelling the reorientation of sea-ice faults as the wind changes direction. Annals of Glaciology, 52 (57). pp. 83-90. ISSN 1727-5644 Article PeerReviewed 2011 ftunivreading 2024-04-17T14:46:07Z A discrete-element model of sea ice is used to study how a 90° change in wind direction alters the pattern of faults generated through mechanical failure of the ice. The sea-ice domain is 400km in size and consists of polygonal floes obtained through a Voronoi tessellation. Initially the floes are frozen together through viscous–elastic joints that can break under sufficient compressive, tensile and shear deformation. A constant wind-stress gradient is applied until the initially frozen ice pack is broken into roughly diamond-shaped aggregates, with crack angles determined by wing-crack formation. Then partial refreezing of the cracks delineating the aggregates is modelled through reduction of their length by a particular fraction, the ice pack deformation is neglected and the wind stress is rotated by 90°. New cracks form, delineating aggregates with a different orientation. Our results show the new crack orientation depends on the refrozen fraction of the initial faults: as this fraction increases, the new cracks gradually rotate to the new wind direction, reaching 90° for fully refrozen faults. Such reorientation is determined by a competition between new cracks forming at a preferential angle determined by the wing-crack theory and at old cracks oriented at a less favourable angle but having higher stresses due to shorter contacts across the joints Article in Journal/Newspaper Annals of Glaciology ice pack Sea ice CentAUR: Central Archive at the University of Reading
institution Open Polar
collection CentAUR: Central Archive at the University of Reading
op_collection_id ftunivreading
language English
description A discrete-element model of sea ice is used to study how a 90° change in wind direction alters the pattern of faults generated through mechanical failure of the ice. The sea-ice domain is 400km in size and consists of polygonal floes obtained through a Voronoi tessellation. Initially the floes are frozen together through viscous–elastic joints that can break under sufficient compressive, tensile and shear deformation. A constant wind-stress gradient is applied until the initially frozen ice pack is broken into roughly diamond-shaped aggregates, with crack angles determined by wing-crack formation. Then partial refreezing of the cracks delineating the aggregates is modelled through reduction of their length by a particular fraction, the ice pack deformation is neglected and the wind stress is rotated by 90°. New cracks form, delineating aggregates with a different orientation. Our results show the new crack orientation depends on the refrozen fraction of the initial faults: as this fraction increases, the new cracks gradually rotate to the new wind direction, reaching 90° for fully refrozen faults. Such reorientation is determined by a competition between new cracks forming at a preferential angle determined by the wing-crack theory and at old cracks oriented at a less favourable angle but having higher stresses due to shorter contacts across the joints
format Article in Journal/Newspaper
author Wilchinsky, A. V.
Feltham, D. L.
Hopkins, M. A.
spellingShingle Wilchinsky, A. V.
Feltham, D. L.
Hopkins, M. A.
Modelling the reorientation of sea-ice faults as the wind changes direction
author_facet Wilchinsky, A. V.
Feltham, D. L.
Hopkins, M. A.
author_sort Wilchinsky, A. V.
title Modelling the reorientation of sea-ice faults as the wind changes direction
title_short Modelling the reorientation of sea-ice faults as the wind changes direction
title_full Modelling the reorientation of sea-ice faults as the wind changes direction
title_fullStr Modelling the reorientation of sea-ice faults as the wind changes direction
title_full_unstemmed Modelling the reorientation of sea-ice faults as the wind changes direction
title_sort modelling the reorientation of sea-ice faults as the wind changes direction
publisher International Glaciological Society
publishDate 2011
url https://centaur.reading.ac.uk/34582/
https://centaur.reading.ac.uk/34582/1/Wilchinsky_etal_2011b.pdf
genre Annals of Glaciology
ice pack
Sea ice
genre_facet Annals of Glaciology
ice pack
Sea ice
op_relation https://centaur.reading.ac.uk/34582/1/Wilchinsky_etal_2011b.pdf
Wilchinsky, A. V., Feltham, D. L. <https://centaur.reading.ac.uk/view/creators/90004991.html> and Hopkins, M. A. (2011) Modelling the reorientation of sea-ice faults as the wind changes direction. Annals of Glaciology, 52 (57). pp. 83-90. ISSN 1727-5644
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