Numerical modelling of ice shelf dynamics

By considering the basic stress equations for a unit volume of ice, a set of differential equations describing ice shelf flow is derived. In view of the lack of basal shear stresses at the bottom of ice shelf a model simulation which is restricted to the horizontal dimensions will not imply substant...

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Published in:Antarctic Science
Main Author: Determann, Jürgen
Format: Article in Journal/Newspaper
Language:English
Published: Cambridge University Press (CUP) 1991
Subjects:
Online Access:https://doi.org/10.1017/s0954102091000226
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0954102091000226
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author Determann, Jürgen
author_facet Determann, Jürgen
author_sort Determann, Jürgen
collection Cambridge University Press
container_issue 2
container_start_page 187
container_title Antarctic Science
container_volume 3
description By considering the basic stress equations for a unit volume of ice, a set of differential equations describing ice shelf flow is derived. In view of the lack of basal shear stresses at the bottom of ice shelf a model simulation which is restricted to the horizontal dimensions will not imply substantial errors. The model is applied to the Filchner-Ronne Ice Shelf, Antarctica, and model equations are solved in terms of finite differences on a 10 × 10 km grid. Present ice thickness data and boundary conditions, i.e. the balance velocities at the grounding line and strain rates at the ice front are entered as input. Using a non-linear Glen-type flow law (n=3) and a constant depth-averaged flow law parameter, representing an ice temperature of −17°C, a convincing velocity field is derived as a solution of the model equations. The model takes into account restrained flow across ice rumples where sufficient field data are available. A diagnostic run reproducing present velocity magnitudes is followed by two prognostic runs, each representing 2000 years of simulation. Transient ice thickness changes are obtained from solving the mass conservation equation. Two different assumptions concerning basal melting rates demonstrate its importance to ice shelf dynamics. Assumptions are: a) no basal melting, b) basal melting rates (−2m a −1 to +3m a −1 ) as derived from model results and geophysical field data.
format Article in Journal/Newspaper
genre Antarc*
Antarctic Science
Antarctica
Filchner Ronne Ice Shelf
Filchner-Ronne Ice Shelf
Ice Shelf
Ronne Ice Shelf
genre_facet Antarc*
Antarctic Science
Antarctica
Filchner Ronne Ice Shelf
Filchner-Ronne Ice Shelf
Ice Shelf
Ronne Ice Shelf
geographic Ronne Ice Shelf
geographic_facet Ronne Ice Shelf
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institution Open Polar
language English
long_lat ENVELOPE(-61.000,-61.000,-78.500,-78.500)
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op_container_end_page 195
op_doi https://doi.org/10.1017/s0954102091000226
op_rights https://www.cambridge.org/core/terms
op_source Antarctic Science
volume 3, issue 2, page 187-195
ISSN 0954-1020 1365-2079
publishDate 1991
publisher Cambridge University Press (CUP)
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spelling crcambridgeupr:10.1017/s0954102091000226 2025-04-20T14:24:32+00:00 Numerical modelling of ice shelf dynamics Determann, Jürgen 1991 https://doi.org/10.1017/s0954102091000226 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0954102091000226 en eng Cambridge University Press (CUP) https://www.cambridge.org/core/terms Antarctic Science volume 3, issue 2, page 187-195 ISSN 0954-1020 1365-2079 journal-article 1991 crcambridgeupr https://doi.org/10.1017/s0954102091000226 2025-04-08T13:12:25Z By considering the basic stress equations for a unit volume of ice, a set of differential equations describing ice shelf flow is derived. In view of the lack of basal shear stresses at the bottom of ice shelf a model simulation which is restricted to the horizontal dimensions will not imply substantial errors. The model is applied to the Filchner-Ronne Ice Shelf, Antarctica, and model equations are solved in terms of finite differences on a 10 × 10 km grid. Present ice thickness data and boundary conditions, i.e. the balance velocities at the grounding line and strain rates at the ice front are entered as input. Using a non-linear Glen-type flow law (n=3) and a constant depth-averaged flow law parameter, representing an ice temperature of −17°C, a convincing velocity field is derived as a solution of the model equations. The model takes into account restrained flow across ice rumples where sufficient field data are available. A diagnostic run reproducing present velocity magnitudes is followed by two prognostic runs, each representing 2000 years of simulation. Transient ice thickness changes are obtained from solving the mass conservation equation. Two different assumptions concerning basal melting rates demonstrate its importance to ice shelf dynamics. Assumptions are: a) no basal melting, b) basal melting rates (−2m a −1 to +3m a −1 ) as derived from model results and geophysical field data. Article in Journal/Newspaper Antarc* Antarctic Science Antarctica Filchner Ronne Ice Shelf Filchner-Ronne Ice Shelf Ice Shelf Ronne Ice Shelf Cambridge University Press Ronne Ice Shelf ENVELOPE(-61.000,-61.000,-78.500,-78.500) Antarctic Science 3 2 187 195
spellingShingle Determann, Jürgen
Numerical modelling of ice shelf dynamics
title Numerical modelling of ice shelf dynamics
title_full Numerical modelling of ice shelf dynamics
title_fullStr Numerical modelling of ice shelf dynamics
title_full_unstemmed Numerical modelling of ice shelf dynamics
title_short Numerical modelling of ice shelf dynamics
title_sort numerical modelling of ice shelf dynamics
url https://doi.org/10.1017/s0954102091000226
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0954102091000226