The evolution of under-ice melt ponds, or double diffusion at the freezing point

In an experimental and theoretical study, we model a phenomenon observed in the summer Arctic, where a fresh-water layer at a temperature of 0°C floats both over a sea-water layer at its freezing point and under an ice layer. Our results show that the ice growth in this system takes place in three p...

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Published in:Journal of Fluid Mechanics
Main Authors: Martin, Seelye, Kauffman, Peter
Format: Article in Journal/Newspaper
Language:English
Published: Cambridge University Press (CUP) 1974
Subjects:
Online Access:http://dx.doi.org/10.1017/s0022112074002527
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022112074002527
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spelling crcambridgeupr:10.1017/s0022112074002527 2024-09-15T18:12:20+00:00 The evolution of under-ice melt ponds, or double diffusion at the freezing point Martin, Seelye Kauffman, Peter 1974 http://dx.doi.org/10.1017/s0022112074002527 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022112074002527 en eng Cambridge University Press (CUP) https://www.cambridge.org/core/terms Journal of Fluid Mechanics volume 64, issue 3, page 507-528 ISSN 0022-1120 1469-7645 journal-article 1974 crcambridgeupr https://doi.org/10.1017/s0022112074002527 2024-07-10T04:04:06Z In an experimental and theoretical study, we model a phenomenon observed in the summer Arctic, where a fresh-water layer at a temperature of 0°C floats both over a sea-water layer at its freezing point and under an ice layer. Our results show that the ice growth in this system takes place in three phases. First, because the fresh-water density decreases upon supercooling, the rapid diffusion of heat relative to salt from the fresh to the salt water causes a density inversion and thereby generates a high Rayleigh number convection in the fresh water. In this convection, supercooled water rises to the ice layer, where it nucleates into thin vertical interlocking ice crystals. When these sheets grow down to the interface, supercooling ceases. Second, the presence of the vertical ice sheets both constrains the temperature T and salinity s to lie on the freezing curve and allows them to diffuse in the vertical. In the interfacial region, the combination of these processes generates a lateral crystal growth, which continues until a horizontal ice sheet forms. Third, because of the T and s gradients in the sea water below this ice sheet, the horizontal sheet both migrates upwards and increases in thickness. From one-dimensional theoretical models of the first two phases, we find that the heat-transfer rates are 5–10 times those calculated for classic thermal diffusion. Article in Journal/Newspaper Ice Sheet Cambridge University Press Journal of Fluid Mechanics 64 3 507 528
institution Open Polar
collection Cambridge University Press
op_collection_id crcambridgeupr
language English
description In an experimental and theoretical study, we model a phenomenon observed in the summer Arctic, where a fresh-water layer at a temperature of 0°C floats both over a sea-water layer at its freezing point and under an ice layer. Our results show that the ice growth in this system takes place in three phases. First, because the fresh-water density decreases upon supercooling, the rapid diffusion of heat relative to salt from the fresh to the salt water causes a density inversion and thereby generates a high Rayleigh number convection in the fresh water. In this convection, supercooled water rises to the ice layer, where it nucleates into thin vertical interlocking ice crystals. When these sheets grow down to the interface, supercooling ceases. Second, the presence of the vertical ice sheets both constrains the temperature T and salinity s to lie on the freezing curve and allows them to diffuse in the vertical. In the interfacial region, the combination of these processes generates a lateral crystal growth, which continues until a horizontal ice sheet forms. Third, because of the T and s gradients in the sea water below this ice sheet, the horizontal sheet both migrates upwards and increases in thickness. From one-dimensional theoretical models of the first two phases, we find that the heat-transfer rates are 5–10 times those calculated for classic thermal diffusion.
format Article in Journal/Newspaper
author Martin, Seelye
Kauffman, Peter
spellingShingle Martin, Seelye
Kauffman, Peter
The evolution of under-ice melt ponds, or double diffusion at the freezing point
author_facet Martin, Seelye
Kauffman, Peter
author_sort Martin, Seelye
title The evolution of under-ice melt ponds, or double diffusion at the freezing point
title_short The evolution of under-ice melt ponds, or double diffusion at the freezing point
title_full The evolution of under-ice melt ponds, or double diffusion at the freezing point
title_fullStr The evolution of under-ice melt ponds, or double diffusion at the freezing point
title_full_unstemmed The evolution of under-ice melt ponds, or double diffusion at the freezing point
title_sort evolution of under-ice melt ponds, or double diffusion at the freezing point
publisher Cambridge University Press (CUP)
publishDate 1974
url http://dx.doi.org/10.1017/s0022112074002527
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022112074002527
genre Ice Sheet
genre_facet Ice Sheet
op_source Journal of Fluid Mechanics
volume 64, issue 3, page 507-528
ISSN 0022-1120 1469-7645
op_rights https://www.cambridge.org/core/terms
op_doi https://doi.org/10.1017/s0022112074002527
container_title Journal of Fluid Mechanics
container_volume 64
container_issue 3
container_start_page 507
op_container_end_page 528
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