Viscous and viscoelastic stress states at the calving front of Antarctic ice shelves

Calving mechanisms are still poorly understood and stress states in the vicinity of ice-shelf fronts are insufficiently known for the development of physically motivated calving laws that match observations. A calving model requires the knowledge of maximum tensile stresses. These stresses depend on...

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Bibliographic Details
Published in:Annals of Glaciology
Main Authors: Julia Christmann, Carolin Plate, Ralf Müller, Angelika Humbert
Format: Article in Journal/Newspaper
Language:English
Published: Cambridge University Press 2016
Subjects:
Online Access:https://doi.org/10.1017/aog.2016.18
https://doaj.org/article/93b23a6612a347708bbd9cc38e3af7d7
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spelling ftdoajarticles:oai:doaj.org/article:93b23a6612a347708bbd9cc38e3af7d7 2023-05-15T13:29:31+02:00 Viscous and viscoelastic stress states at the calving front of Antarctic ice shelves Julia Christmann Carolin Plate Ralf Müller Angelika Humbert 2016-09-01T00:00:00Z https://doi.org/10.1017/aog.2016.18 https://doaj.org/article/93b23a6612a347708bbd9cc38e3af7d7 EN eng Cambridge University Press https://www.cambridge.org/core/product/identifier/S0260305516000185/type/journal_article https://doaj.org/toc/0260-3055 https://doaj.org/toc/1727-5644 doi:10.1017/aog.2016.18 0260-3055 1727-5644 https://doaj.org/article/93b23a6612a347708bbd9cc38e3af7d7 Annals of Glaciology, Vol 57, Pp 10-18 (2016) calving ice-shelves modeling Meteorology. Climatology QC851-999 article 2016 ftdoajarticles https://doi.org/10.1017/aog.2016.18 2023-03-12T01:31:57Z Calving mechanisms are still poorly understood and stress states in the vicinity of ice-shelf fronts are insufficiently known for the development of physically motivated calving laws that match observations. A calving model requires the knowledge of maximum tensile stresses. These stresses depend on different simulation approaches and material models. Therefore, this study compares results of a two-dimensional (2-D) continuum approach using finite elements with results of a one-dimensional (1-D) beam model elaborated in Reeh (1968). A purely viscous model, as well as a viscoelastic Maxwell model, is applied for the 2-D case. The maximum tensile stress usually appears at the top surface of an ice shelf. Its location and magnitude are predominantly influenced by the thickness of the ice shelf and the height of the freeboard, the traction-free part at the ice front. More precisely, doubling the thickness leads to twice the stress maximum, while doubling the freeboard, based on changes of the ice density, results in an increase of the stress maximum by 61%. Poisson's ratio controls the evolution of the maximum stress with time. The viscosity and Young's modulus define the characteristic time of the Maxwell model and thus the time to reach the maximum principal stress. Article in Journal/Newspaper Annals of Glaciology Antarc* Antarctic Ice Shelf Ice Shelves Directory of Open Access Journals: DOAJ Articles Antarctic Annals of Glaciology 57 73 10 18
institution Open Polar
collection Directory of Open Access Journals: DOAJ Articles
op_collection_id ftdoajarticles
language English
topic calving
ice-shelves
modeling
Meteorology. Climatology
QC851-999
spellingShingle calving
ice-shelves
modeling
Meteorology. Climatology
QC851-999
Julia Christmann
Carolin Plate
Ralf Müller
Angelika Humbert
Viscous and viscoelastic stress states at the calving front of Antarctic ice shelves
topic_facet calving
ice-shelves
modeling
Meteorology. Climatology
QC851-999
description Calving mechanisms are still poorly understood and stress states in the vicinity of ice-shelf fronts are insufficiently known for the development of physically motivated calving laws that match observations. A calving model requires the knowledge of maximum tensile stresses. These stresses depend on different simulation approaches and material models. Therefore, this study compares results of a two-dimensional (2-D) continuum approach using finite elements with results of a one-dimensional (1-D) beam model elaborated in Reeh (1968). A purely viscous model, as well as a viscoelastic Maxwell model, is applied for the 2-D case. The maximum tensile stress usually appears at the top surface of an ice shelf. Its location and magnitude are predominantly influenced by the thickness of the ice shelf and the height of the freeboard, the traction-free part at the ice front. More precisely, doubling the thickness leads to twice the stress maximum, while doubling the freeboard, based on changes of the ice density, results in an increase of the stress maximum by 61%. Poisson's ratio controls the evolution of the maximum stress with time. The viscosity and Young's modulus define the characteristic time of the Maxwell model and thus the time to reach the maximum principal stress.
format Article in Journal/Newspaper
author Julia Christmann
Carolin Plate
Ralf Müller
Angelika Humbert
author_facet Julia Christmann
Carolin Plate
Ralf Müller
Angelika Humbert
author_sort Julia Christmann
title Viscous and viscoelastic stress states at the calving front of Antarctic ice shelves
title_short Viscous and viscoelastic stress states at the calving front of Antarctic ice shelves
title_full Viscous and viscoelastic stress states at the calving front of Antarctic ice shelves
title_fullStr Viscous and viscoelastic stress states at the calving front of Antarctic ice shelves
title_full_unstemmed Viscous and viscoelastic stress states at the calving front of Antarctic ice shelves
title_sort viscous and viscoelastic stress states at the calving front of antarctic ice shelves
publisher Cambridge University Press
publishDate 2016
url https://doi.org/10.1017/aog.2016.18
https://doaj.org/article/93b23a6612a347708bbd9cc38e3af7d7
geographic Antarctic
geographic_facet Antarctic
genre Annals of Glaciology
Antarc*
Antarctic
Ice Shelf
Ice Shelves
genre_facet Annals of Glaciology
Antarc*
Antarctic
Ice Shelf
Ice Shelves
op_source Annals of Glaciology, Vol 57, Pp 10-18 (2016)
op_relation https://www.cambridge.org/core/product/identifier/S0260305516000185/type/journal_article
https://doaj.org/toc/0260-3055
https://doaj.org/toc/1727-5644
doi:10.1017/aog.2016.18
0260-3055
1727-5644
https://doaj.org/article/93b23a6612a347708bbd9cc38e3af7d7
op_doi https://doi.org/10.1017/aog.2016.18
container_title Annals of Glaciology
container_volume 57
container_issue 73
container_start_page 10
op_container_end_page 18
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