The evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season

The aim of the present investigation was to provide more insight into the processes affecting the evolution of the englacial temperature distribution at a non-temperate location on a glacier. Measurements were made in the top 10 m of the ice at the summit of Laika Ice Cap (Canadian Arctic) during th...

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Main Authors: Greuell, W., Oerlemans, J.
Format: Conference Object
Language:English
Published: 1989
Subjects:
Online Access:https://dspace.library.uu.nl/handle/1874/22212
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spelling ftunivutrecht:oai:dspace.library.uu.nl:1874/22212 2023-07-23T04:17:58+02:00 The evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season Greuell, W. Oerlemans, J. 1989 image/pdf https://dspace.library.uu.nl/handle/1874/22212 en eng https://dspace.library.uu.nl/handle/1874/22212 info:eu-repo/semantics/OpenAccess Natuur- en Sterrenkunde Article in proceedings 1989 ftunivutrecht 2023-07-01T23:20:28Z The aim of the present investigation was to provide more insight into the processes affecting the evolution of the englacial temperature distribution at a non-temperate location on a glacier. Measurements were made in the top 10 m of the ice at the summit of Laika Ice Cap (Canadian Arctic) during the summer 1975 (by Blatter et al.). This location is in the superimposed ice zone. The model simulation includes calculation of the surface energy fluxes, of radiation penetration, of the englacial temperature and density distribution, and of the formation, penetration and refreezing of melt water. In the first kind of experiments the energy fluxes from the atmosphere were tuned in such a way as to obtain the right amount of ablation. With these energy fluxes as a boundary condition the consequences of melt water penetration and refreezing for the englacial temperature distribution were proofed to be considerable. In the second kind of experiments the measured temperature at the interannual surface was used as boundary condition, and to start with the temperature below the interannual surface could only be affected by conduction. The measured and the calculated temperatures match until melt water penetrates to the interannual surface. Thereafter, calculations give too low temperatures. Most of this energy deficiency will probably be due to radiation penetration, whereas a minor part of it may be caused by melt water penetration into open veins or an error in the assumed interface temperature. Conference Object Arctic Ice cap Polar Ice Cap Utrecht University Repository Arctic
institution Open Polar
collection Utrecht University Repository
op_collection_id ftunivutrecht
language English
topic Natuur- en Sterrenkunde
spellingShingle Natuur- en Sterrenkunde
Greuell, W.
Oerlemans, J.
The evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season
topic_facet Natuur- en Sterrenkunde
description The aim of the present investigation was to provide more insight into the processes affecting the evolution of the englacial temperature distribution at a non-temperate location on a glacier. Measurements were made in the top 10 m of the ice at the summit of Laika Ice Cap (Canadian Arctic) during the summer 1975 (by Blatter et al.). This location is in the superimposed ice zone. The model simulation includes calculation of the surface energy fluxes, of radiation penetration, of the englacial temperature and density distribution, and of the formation, penetration and refreezing of melt water. In the first kind of experiments the energy fluxes from the atmosphere were tuned in such a way as to obtain the right amount of ablation. With these energy fluxes as a boundary condition the consequences of melt water penetration and refreezing for the englacial temperature distribution were proofed to be considerable. In the second kind of experiments the measured temperature at the interannual surface was used as boundary condition, and to start with the temperature below the interannual surface could only be affected by conduction. The measured and the calculated temperatures match until melt water penetrates to the interannual surface. Thereafter, calculations give too low temperatures. Most of this energy deficiency will probably be due to radiation penetration, whereas a minor part of it may be caused by melt water penetration into open veins or an error in the assumed interface temperature.
format Conference Object
author Greuell, W.
Oerlemans, J.
author_facet Greuell, W.
Oerlemans, J.
author_sort Greuell, W.
title The evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season
title_short The evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season
title_full The evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season
title_fullStr The evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season
title_full_unstemmed The evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season
title_sort evolution of the englacial temperature distribution in the superimposed ice zone of a polar ice cap during a summer season
publishDate 1989
url https://dspace.library.uu.nl/handle/1874/22212
geographic Arctic
geographic_facet Arctic
genre Arctic
Ice cap
Polar Ice Cap
genre_facet Arctic
Ice cap
Polar Ice Cap
op_relation https://dspace.library.uu.nl/handle/1874/22212
op_rights info:eu-repo/semantics/OpenAccess
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