Two-Dimensional Spreading and Thickening of Aufeis
Abstract The growth of two-dimensional, or laterally confined (flume), aufeis is shown from laboratory data to depend primarily on seven, independent, dimensionless parameters. During the early, two-dimensional, phase of its growth, aufeis consists of a mixture of ice and water, or ice-water slush,...
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Language: | English |
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Cambridge University Press (CUP)
1990
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Online Access: | http://dx.doi.org/10.1017/s0022143000009412 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000009412 |
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crcambridgeupr:10.1017/s0022143000009412 2024-03-03T08:46:00+00:00 Two-Dimensional Spreading and Thickening of Aufeis Schohl, G.A. Ettema, R. 1990 http://dx.doi.org/10.1017/s0022143000009412 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000009412 en eng Cambridge University Press (CUP) Journal of Glaciology volume 36, issue 123, page 169-178 ISSN 0022-1430 1727-5652 Earth-Surface Processes journal-article 1990 crcambridgeupr https://doi.org/10.1017/s0022143000009412 2024-02-08T08:38:15Z Abstract The growth of two-dimensional, or laterally confined (flume), aufeis is shown from laboratory data to depend primarily on seven, independent, dimensionless parameters. During the early, two-dimensional, phase of its growth, aufeis consists of a mixture of ice and water, or ice-water slush, forming on a frigid base. Its early growth depends on four parameters: those expressing position along aufeis , period of spreading, slope of frigid base over which aufeis forms, and magnitude of heat flux to air from the surface of aufeis relative to latent heat release during freezing. The influences of two of the three remaining parameters, those expressing magnitude of heat flux to air relative to heat flux to frigid base and confined width of aufeis growth, are not felt until after a transition time has passed. The transition time apparently coincides with the beginning of the processes by which the ice-water slush on the surface of aufeis freezes solid. After a slush layer on aufeis begins to freeze solid, a new slush layer forms over its frozen surface. The continuing, cyclic process by which slush layers form and eventually freeze results in the ice laminations that are a feature of aufeis. The influence of the seventh governing parameter, a Reynolds number, cannot be discerned in the laboratory data. Article in Journal/Newspaper Journal of Glaciology Cambridge University Press Journal of Glaciology 36 123 169 178 |
institution |
Open Polar |
collection |
Cambridge University Press |
op_collection_id |
crcambridgeupr |
language |
English |
topic |
Earth-Surface Processes |
spellingShingle |
Earth-Surface Processes Schohl, G.A. Ettema, R. Two-Dimensional Spreading and Thickening of Aufeis |
topic_facet |
Earth-Surface Processes |
description |
Abstract The growth of two-dimensional, or laterally confined (flume), aufeis is shown from laboratory data to depend primarily on seven, independent, dimensionless parameters. During the early, two-dimensional, phase of its growth, aufeis consists of a mixture of ice and water, or ice-water slush, forming on a frigid base. Its early growth depends on four parameters: those expressing position along aufeis , period of spreading, slope of frigid base over which aufeis forms, and magnitude of heat flux to air from the surface of aufeis relative to latent heat release during freezing. The influences of two of the three remaining parameters, those expressing magnitude of heat flux to air relative to heat flux to frigid base and confined width of aufeis growth, are not felt until after a transition time has passed. The transition time apparently coincides with the beginning of the processes by which the ice-water slush on the surface of aufeis freezes solid. After a slush layer on aufeis begins to freeze solid, a new slush layer forms over its frozen surface. The continuing, cyclic process by which slush layers form and eventually freeze results in the ice laminations that are a feature of aufeis. The influence of the seventh governing parameter, a Reynolds number, cannot be discerned in the laboratory data. |
format |
Article in Journal/Newspaper |
author |
Schohl, G.A. Ettema, R. |
author_facet |
Schohl, G.A. Ettema, R. |
author_sort |
Schohl, G.A. |
title |
Two-Dimensional Spreading and Thickening of Aufeis |
title_short |
Two-Dimensional Spreading and Thickening of Aufeis |
title_full |
Two-Dimensional Spreading and Thickening of Aufeis |
title_fullStr |
Two-Dimensional Spreading and Thickening of Aufeis |
title_full_unstemmed |
Two-Dimensional Spreading and Thickening of Aufeis |
title_sort |
two-dimensional spreading and thickening of aufeis |
publisher |
Cambridge University Press (CUP) |
publishDate |
1990 |
url |
http://dx.doi.org/10.1017/s0022143000009412 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000009412 |
genre |
Journal of Glaciology |
genre_facet |
Journal of Glaciology |
op_source |
Journal of Glaciology volume 36, issue 123, page 169-178 ISSN 0022-1430 1727-5652 |
op_doi |
https://doi.org/10.1017/s0022143000009412 |
container_title |
Journal of Glaciology |
container_volume |
36 |
container_issue |
123 |
container_start_page |
169 |
op_container_end_page |
178 |
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1792501800921726976 |