Numerical simulation of the Filchner overflow

The plume of Ice Shelf Water (ISW) flowing into the Weddell Sea over the Filchner sill contributes to the formation of Antarctic Bottom Water. The Filchner overflow is simulated using a hydrostatic, primitive equation three-dimensional ocean model with a 0.5–2 Sv ISW influx above the Filchner sill....

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Main Authors: Alexander V. Wilchinsky, Daniel L. Feltham
Other Authors: The Pennsylvania State University CiteSeerX Archives
Format: Text
Language:English
Published: 2009
Subjects:
Online Access:http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.657.1144
http://centaur.reading.ac.uk/30573/1/Feltham2009.pdf
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spelling ftciteseerx:oai:CiteSeerX.psu:10.1.1.657.1144 2023-05-15T13:43:21+02:00 Numerical simulation of the Filchner overflow Alexander V. Wilchinsky Daniel L. Feltham The Pennsylvania State University CiteSeerX Archives 2009 application/pdf http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.657.1144 http://centaur.reading.ac.uk/30573/1/Feltham2009.pdf en eng http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.657.1144 http://centaur.reading.ac.uk/30573/1/Feltham2009.pdf Metadata may be used without restrictions as long as the oai identifier remains attached to it. http://centaur.reading.ac.uk/30573/1/Feltham2009.pdf text 2009 ftciteseerx 2020-07-19T00:15:42Z The plume of Ice Shelf Water (ISW) flowing into the Weddell Sea over the Filchner sill contributes to the formation of Antarctic Bottom Water. The Filchner overflow is simulated using a hydrostatic, primitive equation three-dimensional ocean model with a 0.5–2 Sv ISW influx above the Filchner sill. The best fit to mooring temperature observations is found with influxes of 0.5 and 1 Sv, below a previous estimate of 1.6 ± 0.5 Sv based on sparse mooring velocities. The plume first moves north over the continental shelf, and then turns west, along slope of the continental shelf break where it breaks up into subplumes and domes, some of which then move downslope. Other subplumes run into the eastern submarine ridge and propagate along the ridge downslope in a chaotic manner. The next, western ridge is crossed by the plume through several paths. Despite a number of discrepancies with observational data, the model reproduces many attributes of the flow. In particular, we argue that the temporal variability shown by the observations can largely be attributed to the unstable structure of the flow, where the temperature fluctuations are determined by the motion of the domes past the moorings. Our sensitivity studies show that while thermobaricity plays a role, its effect is small for the flows considered. Smoothing the Text Antarc* Antarctic Ice Shelf Weddell Sea Unknown Antarctic Weddell Weddell Sea
institution Open Polar
collection Unknown
op_collection_id ftciteseerx
language English
description The plume of Ice Shelf Water (ISW) flowing into the Weddell Sea over the Filchner sill contributes to the formation of Antarctic Bottom Water. The Filchner overflow is simulated using a hydrostatic, primitive equation three-dimensional ocean model with a 0.5–2 Sv ISW influx above the Filchner sill. The best fit to mooring temperature observations is found with influxes of 0.5 and 1 Sv, below a previous estimate of 1.6 ± 0.5 Sv based on sparse mooring velocities. The plume first moves north over the continental shelf, and then turns west, along slope of the continental shelf break where it breaks up into subplumes and domes, some of which then move downslope. Other subplumes run into the eastern submarine ridge and propagate along the ridge downslope in a chaotic manner. The next, western ridge is crossed by the plume through several paths. Despite a number of discrepancies with observational data, the model reproduces many attributes of the flow. In particular, we argue that the temporal variability shown by the observations can largely be attributed to the unstable structure of the flow, where the temperature fluctuations are determined by the motion of the domes past the moorings. Our sensitivity studies show that while thermobaricity plays a role, its effect is small for the flows considered. Smoothing the
author2 The Pennsylvania State University CiteSeerX Archives
format Text
author Alexander V. Wilchinsky
Daniel L. Feltham
spellingShingle Alexander V. Wilchinsky
Daniel L. Feltham
Numerical simulation of the Filchner overflow
author_facet Alexander V. Wilchinsky
Daniel L. Feltham
author_sort Alexander V. Wilchinsky
title Numerical simulation of the Filchner overflow
title_short Numerical simulation of the Filchner overflow
title_full Numerical simulation of the Filchner overflow
title_fullStr Numerical simulation of the Filchner overflow
title_full_unstemmed Numerical simulation of the Filchner overflow
title_sort numerical simulation of the filchner overflow
publishDate 2009
url http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.657.1144
http://centaur.reading.ac.uk/30573/1/Feltham2009.pdf
geographic Antarctic
Weddell
Weddell Sea
geographic_facet Antarctic
Weddell
Weddell Sea
genre Antarc*
Antarctic
Ice Shelf
Weddell Sea
genre_facet Antarc*
Antarctic
Ice Shelf
Weddell Sea
op_source http://centaur.reading.ac.uk/30573/1/Feltham2009.pdf
op_relation http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.657.1144
http://centaur.reading.ac.uk/30573/1/Feltham2009.pdf
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