Simulation of convection at a vertical ice face dissolving into saline water
We investigate the convection and dissolution rate generated when a wall of ice dissolves into seawater under Antarctic Ocean conditions. In direct numerical simulations three coupled interface equations are used to solve for interface temperature, salinity and ablation velocity, along with the boun...
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ftanucanberra:oai:digitalcollections.anu.edu.au:1885/107303 2023-05-15T13:57:32+02:00 Simulation of convection at a vertical ice face dissolving into saline water Gayen, Bishakhdatta Griffiths, Ross W. Kerr, Ross C. 2016-08-25T05:42:36Z http://hdl.handle.net/1885/107303 unknown Cambridge University Press http://purl.org/au-research/grants/arc/DP120102772 http://purl.org/au-research/grants/arc/DP120102744 http://purl.org/au-research/grants/arc/DE140100089 0022-1120 http://hdl.handle.net/1885/107303 © Cambridge University Press 2016 Journal of Fluid Mechanics geophysical and geological flows turbulence simulation turbulent convection Journal article 2016 ftanucanberra 2016-08-29T22:17:43Z We investigate the convection and dissolution rate generated when a wall of ice dissolves into seawater under Antarctic Ocean conditions. In direct numerical simulations three coupled interface equations are used to solve for interface temperature, salinity and ablation velocity, along with the boundary layer flow and transport. The main focus is on ambient water temperatures between −1∘C and 6∘C and salinities around 35 ‰, where diffusion of salt to the ice–water interface depresses the freezing point and enhances heat diffusion to the ice. We show that fluxes of both heat and salt to the interface are significant in governing the dissolution of ice, and the ablation velocity agrees well with experiments and a recent theoretical prediction. The same turbulent flow dynamics and ablation rate are expected to apply at any depth in a deeper ocean water column (after choosing the relevant pressure coefficient for the liquidus temperature). At Grashof numbers currently accessible by direct numerical simulation, turbulence is generated both directly from buoyancy flux and from shear production in the buoyancy-driven boundary layer flow, whereas shear production by the convective flow is expected to be more important at geophysical scales. The momentum balance in the boundary layer is dominated by buoyancy forcing and wall stress, with the latter characterised by a large drag coefficient. Article in Journal/Newspaper Antarc* Antarctic Antarctic Ocean Australian National University: ANU Digital Collections Antarctic Antarctic Ocean |
institution |
Open Polar |
collection |
Australian National University: ANU Digital Collections |
op_collection_id |
ftanucanberra |
language |
unknown |
topic |
geophysical and geological flows turbulence simulation turbulent convection |
spellingShingle |
geophysical and geological flows turbulence simulation turbulent convection Gayen, Bishakhdatta Griffiths, Ross W. Kerr, Ross C. Simulation of convection at a vertical ice face dissolving into saline water |
topic_facet |
geophysical and geological flows turbulence simulation turbulent convection |
description |
We investigate the convection and dissolution rate generated when a wall of ice dissolves into seawater under Antarctic Ocean conditions. In direct numerical simulations three coupled interface equations are used to solve for interface temperature, salinity and ablation velocity, along with the boundary layer flow and transport. The main focus is on ambient water temperatures between −1∘C and 6∘C and salinities around 35 ‰, where diffusion of salt to the ice–water interface depresses the freezing point and enhances heat diffusion to the ice. We show that fluxes of both heat and salt to the interface are significant in governing the dissolution of ice, and the ablation velocity agrees well with experiments and a recent theoretical prediction. The same turbulent flow dynamics and ablation rate are expected to apply at any depth in a deeper ocean water column (after choosing the relevant pressure coefficient for the liquidus temperature). At Grashof numbers currently accessible by direct numerical simulation, turbulence is generated both directly from buoyancy flux and from shear production in the buoyancy-driven boundary layer flow, whereas shear production by the convective flow is expected to be more important at geophysical scales. The momentum balance in the boundary layer is dominated by buoyancy forcing and wall stress, with the latter characterised by a large drag coefficient. |
format |
Article in Journal/Newspaper |
author |
Gayen, Bishakhdatta Griffiths, Ross W. Kerr, Ross C. |
author_facet |
Gayen, Bishakhdatta Griffiths, Ross W. Kerr, Ross C. |
author_sort |
Gayen, Bishakhdatta |
title |
Simulation of convection at a vertical ice face dissolving into saline water |
title_short |
Simulation of convection at a vertical ice face dissolving into saline water |
title_full |
Simulation of convection at a vertical ice face dissolving into saline water |
title_fullStr |
Simulation of convection at a vertical ice face dissolving into saline water |
title_full_unstemmed |
Simulation of convection at a vertical ice face dissolving into saline water |
title_sort |
simulation of convection at a vertical ice face dissolving into saline water |
publisher |
Cambridge University Press |
publishDate |
2016 |
url |
http://hdl.handle.net/1885/107303 |
geographic |
Antarctic Antarctic Ocean |
geographic_facet |
Antarctic Antarctic Ocean |
genre |
Antarc* Antarctic Antarctic Ocean |
genre_facet |
Antarc* Antarctic Antarctic Ocean |
op_source |
Journal of Fluid Mechanics |
op_relation |
http://purl.org/au-research/grants/arc/DP120102772 http://purl.org/au-research/grants/arc/DP120102744 http://purl.org/au-research/grants/arc/DE140100089 0022-1120 http://hdl.handle.net/1885/107303 |
op_rights |
© Cambridge University Press 2016 |
_version_ |
1766265200315465728 |