Comparison of thermodynamics solvers in the polythermal ice sheet model SICOPOLIS

In order to model the thermal structure of polythermal ice sheets accurately, energy-conserving schemes and correct tracking of the coldetemperate transition surface (CTS) are necessary. We compare four different thermodynamics solvers in the ice sheet model SICOPOLIS. Two exist already, namely a tw...

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Published in:Polar Science
Main Authors: Greve, Ralf, Blatter, Heinz
Format: Article in Journal/Newspaper
Language:English
Published: Elsevier
Subjects:
Online Access:http://hdl.handle.net/2115/68069
https://doi.org/10.1016/j.polar.2015.12.004
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record_format openpolar
spelling fthokunivhus:oai:eprints.lib.hokudai.ac.jp:2115/68069 2023-11-05T03:42:41+01:00 Comparison of thermodynamics solvers in the polythermal ice sheet model SICOPOLIS Greve, Ralf Blatter, Heinz http://hdl.handle.net/2115/68069 https://doi.org/10.1016/j.polar.2015.12.004 eng eng Elsevier http://hdl.handle.net/2115/68069 Polar Science, 10(1): 11-23 http://dx.doi.org/10.1016/j.polar.2015.12.004 ©2016, Elsevier. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/ http://creativecommons.org/licenses/by-nc-nd/4.0/ Ice sheet Thermodynamics Polythermal ice Enthalpy method Modeling article (author version) fthokunivhus https://doi.org/10.1016/j.polar.2015.12.004 2023-10-06T00:06:41Z In order to model the thermal structure of polythermal ice sheets accurately, energy-conserving schemes and correct tracking of the coldetemperate transition surface (CTS) are necessary. We compare four different thermodynamics solvers in the ice sheet model SICOPOLIS. Two exist already, namely a twolayer polythermal scheme (POLY) and a single-phase cold-ice scheme (COLD), while the other two are newly-implemented, one-layer enthalpy schemes, namely a conventional scheme (ENTC) and a meltingCTS scheme (ENTM). The comparison uses scenarios of the EISMINT Phase 2 Simplified Geometry Experiments (Payne et al., 2000, J. Glaciol. 46, 227-238). The POLY scheme is used as a reference against which the performance of the other schemes is tested. Both the COLD scheme and the ENTC scheme fail to produce a continuous temperature gradient across the CTS, which is explicitly enforced by the ENTM scheme. ENTM is more precise than ENTC for determining the position of the CTS, while the performance of both schemes is good for the temperature/water-content profiles in the entire ice column. Therefore, the one-layer enthalpy schemes ENTC and ENTM are viable, easier implementable alternatives to the POLY scheme with its need to handle two different numerical domains for cold and temperate ice. (C) 2016 Elsevier B.V. and NIPR. All rights reserved. Article in Journal/Newspaper Ice Sheet Polar Science Polar Science Hokkaido University Collection of Scholarly and Academic Papers (HUSCAP) Polar Science 10 1 11 23
institution Open Polar
collection Hokkaido University Collection of Scholarly and Academic Papers (HUSCAP)
op_collection_id fthokunivhus
language English
topic Ice sheet
Thermodynamics
Polythermal ice
Enthalpy method
Modeling
spellingShingle Ice sheet
Thermodynamics
Polythermal ice
Enthalpy method
Modeling
Greve, Ralf
Blatter, Heinz
Comparison of thermodynamics solvers in the polythermal ice sheet model SICOPOLIS
topic_facet Ice sheet
Thermodynamics
Polythermal ice
Enthalpy method
Modeling
description In order to model the thermal structure of polythermal ice sheets accurately, energy-conserving schemes and correct tracking of the coldetemperate transition surface (CTS) are necessary. We compare four different thermodynamics solvers in the ice sheet model SICOPOLIS. Two exist already, namely a twolayer polythermal scheme (POLY) and a single-phase cold-ice scheme (COLD), while the other two are newly-implemented, one-layer enthalpy schemes, namely a conventional scheme (ENTC) and a meltingCTS scheme (ENTM). The comparison uses scenarios of the EISMINT Phase 2 Simplified Geometry Experiments (Payne et al., 2000, J. Glaciol. 46, 227-238). The POLY scheme is used as a reference against which the performance of the other schemes is tested. Both the COLD scheme and the ENTC scheme fail to produce a continuous temperature gradient across the CTS, which is explicitly enforced by the ENTM scheme. ENTM is more precise than ENTC for determining the position of the CTS, while the performance of both schemes is good for the temperature/water-content profiles in the entire ice column. Therefore, the one-layer enthalpy schemes ENTC and ENTM are viable, easier implementable alternatives to the POLY scheme with its need to handle two different numerical domains for cold and temperate ice. (C) 2016 Elsevier B.V. and NIPR. All rights reserved.
format Article in Journal/Newspaper
author Greve, Ralf
Blatter, Heinz
author_facet Greve, Ralf
Blatter, Heinz
author_sort Greve, Ralf
title Comparison of thermodynamics solvers in the polythermal ice sheet model SICOPOLIS
title_short Comparison of thermodynamics solvers in the polythermal ice sheet model SICOPOLIS
title_full Comparison of thermodynamics solvers in the polythermal ice sheet model SICOPOLIS
title_fullStr Comparison of thermodynamics solvers in the polythermal ice sheet model SICOPOLIS
title_full_unstemmed Comparison of thermodynamics solvers in the polythermal ice sheet model SICOPOLIS
title_sort comparison of thermodynamics solvers in the polythermal ice sheet model sicopolis
publisher Elsevier
url http://hdl.handle.net/2115/68069
https://doi.org/10.1016/j.polar.2015.12.004
genre Ice Sheet
Polar Science
Polar Science
genre_facet Ice Sheet
Polar Science
Polar Science
op_relation http://hdl.handle.net/2115/68069
Polar Science, 10(1): 11-23
http://dx.doi.org/10.1016/j.polar.2015.12.004
op_rights ©2016, Elsevier. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/
http://creativecommons.org/licenses/by-nc-nd/4.0/
op_doi https://doi.org/10.1016/j.polar.2015.12.004
container_title Polar Science
container_volume 10
container_issue 1
container_start_page 11
op_container_end_page 23
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