A First Simple Model for Periodically Self-Surging Glaciers

A two-dimensional model of glacier flow is presented which includes periodical surging as a natural phenomenon for a certain class of glaciers. The input consists of the bedrock and balance profiles along the glacier, together with the ice flow properties and a frictional lubrication factor. The bas...

Full description

Bibliographic Details
Published in:Journal of Glaciology
Main Author: Budd, W. F.
Format: Article in Journal/Newspaper
Language:English
Published: Cambridge University Press (CUP) 1975
Subjects:
Online Access:http://dx.doi.org/10.1017/s0022143000013344
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000013344
id crcambridgeupr:10.1017/s0022143000013344
record_format openpolar
spelling crcambridgeupr:10.1017/s0022143000013344 2024-09-15T18:15:38+00:00 A First Simple Model for Periodically Self-Surging Glaciers Budd, W. F. 1975 http://dx.doi.org/10.1017/s0022143000013344 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000013344 en eng Cambridge University Press (CUP) Journal of Glaciology volume 14, issue 70, page 3-21 ISSN 0022-1430 1727-5652 journal-article 1975 crcambridgeupr https://doi.org/10.1017/s0022143000013344 2024-07-31T04:03:56Z A two-dimensional model of glacier flow is presented which includes periodical surging as a natural phenomenon for a certain class of glaciers. The input consists of the bedrock and balance profiles along the glacier, together with the ice flow properties and a frictional lubrication factor. The basal stress is determined from the condition of gross equilibrium for the whole glacier, together with the distribution of the frictional lubrication from energy dissipation along the glacier. The difference between the basal stress and the down-slope stress of the glaciers produces longitudinal strain-rates which determine the basal sliding velocity. Since the velocity is also involved in the frictional lubrication, feed-back develops between the basal stress and sliding velocity. For a given lubrication factor, a critical stage can be reached for which the velocity becomes sufficiently high to lower the basal stress, enough to cause very high velocities to develop. The model thus gives rise to three classes of glaciers with two modes of flow. “Ordinary” glaciers do not have sufficient mass flux, for the given bedrock profile, to go beyond the “slow mode” in which the basal stress and velocity increase together as the glacier builds up to steady state. “Fast” glaciers have sufficient flux to remain continuously in the “fast mode” with high velocities and relatively low basal stress. “Surging” glaciers have sufficient flux to reach the fast mode but not sufficient to maintain it, and thus develop a periodically oscillating state between the fast and slow modes with gradual build up and rapid drainage. Sample results are presented for models of a typical large valley surging glacier and for a very high-speed surging glacier. Article in Journal/Newspaper Journal of Glaciology Cambridge University Press Journal of Glaciology 14 70 3 21
institution Open Polar
collection Cambridge University Press
op_collection_id crcambridgeupr
language English
description A two-dimensional model of glacier flow is presented which includes periodical surging as a natural phenomenon for a certain class of glaciers. The input consists of the bedrock and balance profiles along the glacier, together with the ice flow properties and a frictional lubrication factor. The basal stress is determined from the condition of gross equilibrium for the whole glacier, together with the distribution of the frictional lubrication from energy dissipation along the glacier. The difference between the basal stress and the down-slope stress of the glaciers produces longitudinal strain-rates which determine the basal sliding velocity. Since the velocity is also involved in the frictional lubrication, feed-back develops between the basal stress and sliding velocity. For a given lubrication factor, a critical stage can be reached for which the velocity becomes sufficiently high to lower the basal stress, enough to cause very high velocities to develop. The model thus gives rise to three classes of glaciers with two modes of flow. “Ordinary” glaciers do not have sufficient mass flux, for the given bedrock profile, to go beyond the “slow mode” in which the basal stress and velocity increase together as the glacier builds up to steady state. “Fast” glaciers have sufficient flux to remain continuously in the “fast mode” with high velocities and relatively low basal stress. “Surging” glaciers have sufficient flux to reach the fast mode but not sufficient to maintain it, and thus develop a periodically oscillating state between the fast and slow modes with gradual build up and rapid drainage. Sample results are presented for models of a typical large valley surging glacier and for a very high-speed surging glacier.
format Article in Journal/Newspaper
author Budd, W. F.
spellingShingle Budd, W. F.
A First Simple Model for Periodically Self-Surging Glaciers
author_facet Budd, W. F.
author_sort Budd, W. F.
title A First Simple Model for Periodically Self-Surging Glaciers
title_short A First Simple Model for Periodically Self-Surging Glaciers
title_full A First Simple Model for Periodically Self-Surging Glaciers
title_fullStr A First Simple Model for Periodically Self-Surging Glaciers
title_full_unstemmed A First Simple Model for Periodically Self-Surging Glaciers
title_sort first simple model for periodically self-surging glaciers
publisher Cambridge University Press (CUP)
publishDate 1975
url http://dx.doi.org/10.1017/s0022143000013344
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000013344
genre Journal of Glaciology
genre_facet Journal of Glaciology
op_source Journal of Glaciology
volume 14, issue 70, page 3-21
ISSN 0022-1430 1727-5652
op_doi https://doi.org/10.1017/s0022143000013344
container_title Journal of Glaciology
container_volume 14
container_issue 70
container_start_page 3
op_container_end_page 21
_version_ 1810453531495235584