Turbulent heat exchange between water and ice at an evolving ice-water interface

We conduct laboratory experiments on the time evolution of an ice layer cooled from below and subjected to a turbulent shear flow of warm water from above. Our study is motivated by observations of warm water intrusion into the ocean cavity under Antarctic ice shelves, accelerating the melting of th...

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Main Authors: Ramudu, Eshwan, Hirsh, Benjamin Henry, Olson, Peter, Gnanadesikan, Anand
Format: Text
Language:unknown
Published: arXiv 2015
Subjects:
Online Access:https://dx.doi.org/10.48550/arxiv.1512.00303
https://arxiv.org/abs/1512.00303
id ftdatacite:10.48550/arxiv.1512.00303
record_format openpolar
spelling ftdatacite:10.48550/arxiv.1512.00303 2023-05-15T13:33:03+02:00 Turbulent heat exchange between water and ice at an evolving ice-water interface Ramudu, Eshwan Hirsh, Benjamin Henry Olson, Peter Gnanadesikan, Anand 2015 https://dx.doi.org/10.48550/arxiv.1512.00303 https://arxiv.org/abs/1512.00303 unknown arXiv https://dx.doi.org/10.1017/jfm.2016.321 arXiv.org perpetual, non-exclusive license http://arxiv.org/licenses/nonexclusive-distrib/1.0/ Fluid Dynamics physics.flu-dyn FOS Physical sciences article-journal Article ScholarlyArticle Text 2015 ftdatacite https://doi.org/10.48550/arxiv.1512.00303 https://doi.org/10.1017/jfm.2016.321 2022-04-01T11:32:48Z We conduct laboratory experiments on the time evolution of an ice layer cooled from below and subjected to a turbulent shear flow of warm water from above. Our study is motivated by observations of warm water intrusion into the ocean cavity under Antarctic ice shelves, accelerating the melting of their basal surfaces. The strength of the applied turbulent shear flow in our experiments is represented in terms of its Reynolds number $\textit{Re}$, which is varied over the range $2.0\times10^3 \le \textit{Re} \le 1.0\times10^4$. Depending on the water temperature, partial transient melting of the ice occurs at the lower end of this range of $\textit{Re}$ and complete transient melting of the ice occurs at the higher end. Following these episodes of transient melting, the ice reforms at a rate that is independent of $\textit{Re}$. We fit our experimental measurements of ice thickness and temperature to a one-dimensional model for the evolution of the ice thickness in which the turbulent heat transfer is parameterized in terms of the friction velocity of the shear flow. The melting mechanism we investigate in our experiments can easily account for the basal melting rate of Pine Island Glacier ice shelf inferred from observations. Text Antarc* Antarctic Ice Shelf Ice Shelves Pine Island Glacier DataCite Metadata Store (German National Library of Science and Technology) Antarctic Pine Island Glacier ENVELOPE(-101.000,-101.000,-75.000,-75.000)
institution Open Polar
collection DataCite Metadata Store (German National Library of Science and Technology)
op_collection_id ftdatacite
language unknown
topic Fluid Dynamics physics.flu-dyn
FOS Physical sciences
spellingShingle Fluid Dynamics physics.flu-dyn
FOS Physical sciences
Ramudu, Eshwan
Hirsh, Benjamin Henry
Olson, Peter
Gnanadesikan, Anand
Turbulent heat exchange between water and ice at an evolving ice-water interface
topic_facet Fluid Dynamics physics.flu-dyn
FOS Physical sciences
description We conduct laboratory experiments on the time evolution of an ice layer cooled from below and subjected to a turbulent shear flow of warm water from above. Our study is motivated by observations of warm water intrusion into the ocean cavity under Antarctic ice shelves, accelerating the melting of their basal surfaces. The strength of the applied turbulent shear flow in our experiments is represented in terms of its Reynolds number $\textit{Re}$, which is varied over the range $2.0\times10^3 \le \textit{Re} \le 1.0\times10^4$. Depending on the water temperature, partial transient melting of the ice occurs at the lower end of this range of $\textit{Re}$ and complete transient melting of the ice occurs at the higher end. Following these episodes of transient melting, the ice reforms at a rate that is independent of $\textit{Re}$. We fit our experimental measurements of ice thickness and temperature to a one-dimensional model for the evolution of the ice thickness in which the turbulent heat transfer is parameterized in terms of the friction velocity of the shear flow. The melting mechanism we investigate in our experiments can easily account for the basal melting rate of Pine Island Glacier ice shelf inferred from observations.
format Text
author Ramudu, Eshwan
Hirsh, Benjamin Henry
Olson, Peter
Gnanadesikan, Anand
author_facet Ramudu, Eshwan
Hirsh, Benjamin Henry
Olson, Peter
Gnanadesikan, Anand
author_sort Ramudu, Eshwan
title Turbulent heat exchange between water and ice at an evolving ice-water interface
title_short Turbulent heat exchange between water and ice at an evolving ice-water interface
title_full Turbulent heat exchange between water and ice at an evolving ice-water interface
title_fullStr Turbulent heat exchange between water and ice at an evolving ice-water interface
title_full_unstemmed Turbulent heat exchange between water and ice at an evolving ice-water interface
title_sort turbulent heat exchange between water and ice at an evolving ice-water interface
publisher arXiv
publishDate 2015
url https://dx.doi.org/10.48550/arxiv.1512.00303
https://arxiv.org/abs/1512.00303
long_lat ENVELOPE(-101.000,-101.000,-75.000,-75.000)
geographic Antarctic
Pine Island Glacier
geographic_facet Antarctic
Pine Island Glacier
genre Antarc*
Antarctic
Ice Shelf
Ice Shelves
Pine Island Glacier
genre_facet Antarc*
Antarctic
Ice Shelf
Ice Shelves
Pine Island Glacier
op_relation https://dx.doi.org/10.1017/jfm.2016.321
op_rights arXiv.org perpetual, non-exclusive license
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
op_doi https://doi.org/10.48550/arxiv.1512.00303
https://doi.org/10.1017/jfm.2016.321
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