Modelling flow in the porous bottom of the Barents Sea shelf

In their recent paper, Węsławski et al. (2012) showed that theSvalbardbanken area of the Barents Sea is characterized by a high organiccarbon settlement to the permeable sea bed, which consists of gravel andshell fragments of glacial origin.In the present paper, which can be considered as a suppl...

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Main Author: Stanisław R. Massel
Format: Article
Language:English
Published: Elsevier 2013-02-01
Series:Oceanologia
Subjects:
Online Access:http://www.iopan.gda.pl/oceanologia/55_1.html#A6
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spelling doaj-2bec29881d404e1483fd76de6d577bc02020-11-24T22:45:10ZengElsevierOceanologia0078-32342013-02-01551129146Modelling flow in the porous bottom of the Barents Sea shelf Stanisław R. MasselIn their recent paper, Węsławski et al. (2012) showed that theSvalbardbanken area of the Barents Sea is characterized by a high organiccarbon settlement to the permeable sea bed, which consists of gravel andshell fragments of glacial origin.In the present paper, which can be considered as a supplement to the Węsławskiet al. paper, two potential hydrodynamic mechanisms of downwardpore water transport into porous media are discussed in detail.In particular, estimated statistical characteristics of the pore waterflow, induced by storm surface waves, indicate that the dischargeof water flow can be substantial, even at large water depths.During stormy weather (wind velocity V=15 m s<sup>-1</sup> and windfetch X =200 km) as much as 117.2 and 26.1 m<sup>3</sup> hour<sup>-1</sup> ofwater filter through the upper 5 m of the shell pit at waterdepths of 30 and 50 m respectively. For a porous layer ofgreater thickness, the mean flow discharge is even bigger.<br>     The second possible mechanism of flow penetration in the porous layeris based on the concept of geostrophic flow and spiral formation withinthe Ekman layer. Assuming that the current velocity in the near-bottomwater layer is <i>ū</i> = 1 m, the resulting mean dischargethrough this layer becomes as large as 0.99 and 0.09 m<sup>3</sup> s<sup>-1</sup>for downstream and transverse flows respectively.http://www.iopan.gda.pl/oceanologia/55_1.html#A6Porous mediaSurface wavesTidesEkman layer
collection DOAJ
language English
format Article
sources DOAJ
author Stanisław R. Massel
spellingShingle Stanisław R. Massel
Modelling flow in the porous bottom of the Barents Sea shelf
Oceanologia
Porous media
Surface waves
Tides
Ekman layer
author_facet Stanisław R. Massel
author_sort Stanisław R. Massel
title Modelling flow in the porous bottom of the Barents Sea shelf
title_short Modelling flow in the porous bottom of the Barents Sea shelf
title_full Modelling flow in the porous bottom of the Barents Sea shelf
title_fullStr Modelling flow in the porous bottom of the Barents Sea shelf
title_full_unstemmed Modelling flow in the porous bottom of the Barents Sea shelf
title_sort modelling flow in the porous bottom of the barents sea shelf
publisher Elsevier
series Oceanologia
issn 0078-3234
publishDate 2013-02-01
description In their recent paper, Węsławski et al. (2012) showed that theSvalbardbanken area of the Barents Sea is characterized by a high organiccarbon settlement to the permeable sea bed, which consists of gravel andshell fragments of glacial origin.In the present paper, which can be considered as a supplement to the Węsławskiet al. paper, two potential hydrodynamic mechanisms of downwardpore water transport into porous media are discussed in detail.In particular, estimated statistical characteristics of the pore waterflow, induced by storm surface waves, indicate that the dischargeof water flow can be substantial, even at large water depths.During stormy weather (wind velocity V=15 m s<sup>-1</sup> and windfetch X =200 km) as much as 117.2 and 26.1 m<sup>3</sup> hour<sup>-1</sup> ofwater filter through the upper 5 m of the shell pit at waterdepths of 30 and 50 m respectively. For a porous layer ofgreater thickness, the mean flow discharge is even bigger.<br>     The second possible mechanism of flow penetration in the porous layeris based on the concept of geostrophic flow and spiral formation withinthe Ekman layer. Assuming that the current velocity in the near-bottomwater layer is <i>ū</i> = 1 m, the resulting mean dischargethrough this layer becomes as large as 0.99 and 0.09 m<sup>3</sup> s<sup>-1</sup>for downstream and transverse flows respectively.
topic Porous media
Surface waves
Tides
Ekman layer
url http://www.iopan.gda.pl/oceanologia/55_1.html#A6
work_keys_str_mv AT stanisławrmassel modellingflowintheporousbottomofthebarentsseashelf
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