Crossover scaling phenomena for glaciers and ice caps

ABSTRACT While the terms ‘glacier’ and ‘ice cap’ have distinct morphological meanings, no easily defined boundary or transition distinguishes one from the other. Despite this, the exponent of the power law function relating volume to surface area differs sharply for glaciers and ice caps, suggesting...

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Published in:Journal of Glaciology
Main Authors: BAHR, DAVID B., PFEFFER, W. TAD
Format: Article in Journal/Newspaper
Language:English
Published: Cambridge University Press (CUP) 2016
Subjects:
Online Access:http://dx.doi.org/10.1017/jog.2016.6
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S002214301600006X
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spelling crcambridgeupr:10.1017/jog.2016.6 2024-03-03T08:45:19+00:00 Crossover scaling phenomena for glaciers and ice caps BAHR, DAVID B. PFEFFER, W. TAD 2016 http://dx.doi.org/10.1017/jog.2016.6 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S002214301600006X en eng Cambridge University Press (CUP) http://creativecommons.org/licenses/by/4.0/ Journal of Glaciology volume 62, issue 232, page 299-309 ISSN 0022-1430 1727-5652 Earth-Surface Processes journal-article 2016 crcambridgeupr https://doi.org/10.1017/jog.2016.6 2024-02-08T08:33:09Z ABSTRACT While the terms ‘glacier’ and ‘ice cap’ have distinct morphological meanings, no easily defined boundary or transition distinguishes one from the other. Despite this, the exponent of the power law function relating volume to surface area differs sharply for glaciers and ice caps, suggesting a fundamental distinction beyond a smoothly transitioning morphology. A standard percolation technique from statistical physics is used to show that valley glaciers are in fact differentiated from ice caps by an abrupt geometric transition. The crossover is a function of increasing glacier thickness, but it owes its existence more to the nature of the underlying bedrock topography than to specifics of glacier mechanics: the crossover is caused by a switch from directed flow that is constrained by surrounding bedrock topography to unconstrained radial flow of thicker ice that has subsumed the topography. The crossover phenomenon is nonlinear and rapid so that few if any glaciers will have geometries or dynamics that blend the two extremes. The exponents of scaling relationships change abruptly at the crossover from one regime to another; in particular, the volume/area scaling exponent will switch from γ = 1.375 for glaciers to γ = 1.25 for ice caps, with few, if any, ice bodies having exponents that fall between these values. Article in Journal/Newspaper Ice cap Journal of Glaciology Cambridge University Press Journal of Glaciology 62 232 299 309
institution Open Polar
collection Cambridge University Press
op_collection_id crcambridgeupr
language English
topic Earth-Surface Processes
spellingShingle Earth-Surface Processes
BAHR, DAVID B.
PFEFFER, W. TAD
Crossover scaling phenomena for glaciers and ice caps
topic_facet Earth-Surface Processes
description ABSTRACT While the terms ‘glacier’ and ‘ice cap’ have distinct morphological meanings, no easily defined boundary or transition distinguishes one from the other. Despite this, the exponent of the power law function relating volume to surface area differs sharply for glaciers and ice caps, suggesting a fundamental distinction beyond a smoothly transitioning morphology. A standard percolation technique from statistical physics is used to show that valley glaciers are in fact differentiated from ice caps by an abrupt geometric transition. The crossover is a function of increasing glacier thickness, but it owes its existence more to the nature of the underlying bedrock topography than to specifics of glacier mechanics: the crossover is caused by a switch from directed flow that is constrained by surrounding bedrock topography to unconstrained radial flow of thicker ice that has subsumed the topography. The crossover phenomenon is nonlinear and rapid so that few if any glaciers will have geometries or dynamics that blend the two extremes. The exponents of scaling relationships change abruptly at the crossover from one regime to another; in particular, the volume/area scaling exponent will switch from γ = 1.375 for glaciers to γ = 1.25 for ice caps, with few, if any, ice bodies having exponents that fall between these values.
format Article in Journal/Newspaper
author BAHR, DAVID B.
PFEFFER, W. TAD
author_facet BAHR, DAVID B.
PFEFFER, W. TAD
author_sort BAHR, DAVID B.
title Crossover scaling phenomena for glaciers and ice caps
title_short Crossover scaling phenomena for glaciers and ice caps
title_full Crossover scaling phenomena for glaciers and ice caps
title_fullStr Crossover scaling phenomena for glaciers and ice caps
title_full_unstemmed Crossover scaling phenomena for glaciers and ice caps
title_sort crossover scaling phenomena for glaciers and ice caps
publisher Cambridge University Press (CUP)
publishDate 2016
url http://dx.doi.org/10.1017/jog.2016.6
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S002214301600006X
genre Ice cap
Journal of Glaciology
genre_facet Ice cap
Journal of Glaciology
op_source Journal of Glaciology
volume 62, issue 232, page 299-309
ISSN 0022-1430 1727-5652
op_rights http://creativecommons.org/licenses/by/4.0/
op_doi https://doi.org/10.1017/jog.2016.6
container_title Journal of Glaciology
container_volume 62
container_issue 232
container_start_page 299
op_container_end_page 309
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