A parameter model of gas exchange for the seasonal sea ice zone

Carbon budgets for the polar oceans require better constraint on air–sea gas exchange in the sea ice zone (SIZ). Here, we utilize advances in the theory of turbulence, mixing and air–sea flux in the ice–ocean boundary layer (IOBL) to formulate a simple model for gas exchange when the surface ocean i...

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Main Authors: Loose, B., McGillis, Wade R., Perovich, D., Zappa, Christopher J., Schlosser, Peter
Format: Text
Language:unknown
Published: Columbia University 2014
Subjects:
Online Access:https://dx.doi.org/10.7916/d81n810b
https://academiccommons.columbia.edu/doi/10.7916/D81N810B
id ftdatacite:10.7916/d81n810b
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spelling ftdatacite:10.7916/d81n810b 2023-05-15T15:13:01+02:00 A parameter model of gas exchange for the seasonal sea ice zone Loose, B. McGillis, Wade R. Perovich, D. Zappa, Christopher J. Schlosser, Peter 2014 https://dx.doi.org/10.7916/d81n810b https://academiccommons.columbia.edu/doi/10.7916/D81N810B unknown Columbia University https://dx.doi.org/10.5194/os-10-17-2014 Ocean-atmosphere interaction Atmospheric turbulence--Mathematical models Sea ice Oceanography Mathematics Meteorology Text Articles article-journal ScholarlyArticle 2014 ftdatacite https://doi.org/10.7916/d81n810b https://doi.org/10.5194/os-10-17-2014 2021-11-05T12:55:41Z Carbon budgets for the polar oceans require better constraint on air–sea gas exchange in the sea ice zone (SIZ). Here, we utilize advances in the theory of turbulence, mixing and air–sea flux in the ice–ocean boundary layer (IOBL) to formulate a simple model for gas exchange when the surface ocean is partially covered by sea ice. The gas transfer velocity (k) is related to shear-driven and convection-driven turbulence in the aqueous mass boundary layer, and to the mean-squared wave slope at the air–sea interface. We use the model to estimate k along the drift track of ice-tethered profilers (ITPs) in the Arctic. Individual estimates of daily-averaged k from ITP drifts ranged between 1.1 and 22 m d−1, and the fraction of open water (f) ranged from 0 to 0.83. Converted to area-weighted effective transfer velocities (keff), the minimum value of keff was 10−55 m d−1 near f = 0 with values exceeding keff = 5 m d−1 at f = 0.4. The model indicates that effects from shear and convection in the sea ice zone contribute an additional 40% to the magnitude of keff, beyond what would be predicted from an estimate of keff based solely upon a wind speed parameterization. Although the ultimate scaling relationship for gas exchange in the sea ice zone will require validation in laboratory and field studies, the basic parameter model described here demonstrates that it is feasible to formulate estimates of k based upon properties of the IOBL using data sources that presently exist. Text Arctic Sea ice DataCite Metadata Store (German National Library of Science and Technology) Arctic
institution Open Polar
collection DataCite Metadata Store (German National Library of Science and Technology)
op_collection_id ftdatacite
language unknown
topic Ocean-atmosphere interaction
Atmospheric turbulence--Mathematical models
Sea ice
Oceanography
Mathematics
Meteorology
spellingShingle Ocean-atmosphere interaction
Atmospheric turbulence--Mathematical models
Sea ice
Oceanography
Mathematics
Meteorology
Loose, B.
McGillis, Wade R.
Perovich, D.
Zappa, Christopher J.
Schlosser, Peter
A parameter model of gas exchange for the seasonal sea ice zone
topic_facet Ocean-atmosphere interaction
Atmospheric turbulence--Mathematical models
Sea ice
Oceanography
Mathematics
Meteorology
description Carbon budgets for the polar oceans require better constraint on air–sea gas exchange in the sea ice zone (SIZ). Here, we utilize advances in the theory of turbulence, mixing and air–sea flux in the ice–ocean boundary layer (IOBL) to formulate a simple model for gas exchange when the surface ocean is partially covered by sea ice. The gas transfer velocity (k) is related to shear-driven and convection-driven turbulence in the aqueous mass boundary layer, and to the mean-squared wave slope at the air–sea interface. We use the model to estimate k along the drift track of ice-tethered profilers (ITPs) in the Arctic. Individual estimates of daily-averaged k from ITP drifts ranged between 1.1 and 22 m d−1, and the fraction of open water (f) ranged from 0 to 0.83. Converted to area-weighted effective transfer velocities (keff), the minimum value of keff was 10−55 m d−1 near f = 0 with values exceeding keff = 5 m d−1 at f = 0.4. The model indicates that effects from shear and convection in the sea ice zone contribute an additional 40% to the magnitude of keff, beyond what would be predicted from an estimate of keff based solely upon a wind speed parameterization. Although the ultimate scaling relationship for gas exchange in the sea ice zone will require validation in laboratory and field studies, the basic parameter model described here demonstrates that it is feasible to formulate estimates of k based upon properties of the IOBL using data sources that presently exist.
format Text
author Loose, B.
McGillis, Wade R.
Perovich, D.
Zappa, Christopher J.
Schlosser, Peter
author_facet Loose, B.
McGillis, Wade R.
Perovich, D.
Zappa, Christopher J.
Schlosser, Peter
author_sort Loose, B.
title A parameter model of gas exchange for the seasonal sea ice zone
title_short A parameter model of gas exchange for the seasonal sea ice zone
title_full A parameter model of gas exchange for the seasonal sea ice zone
title_fullStr A parameter model of gas exchange for the seasonal sea ice zone
title_full_unstemmed A parameter model of gas exchange for the seasonal sea ice zone
title_sort parameter model of gas exchange for the seasonal sea ice zone
publisher Columbia University
publishDate 2014
url https://dx.doi.org/10.7916/d81n810b
https://academiccommons.columbia.edu/doi/10.7916/D81N810B
geographic Arctic
geographic_facet Arctic
genre Arctic
Sea ice
genre_facet Arctic
Sea ice
op_relation https://dx.doi.org/10.5194/os-10-17-2014
op_doi https://doi.org/10.7916/d81n810b
https://doi.org/10.5194/os-10-17-2014
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