English
 
Privacy Policy Disclaimer
  Advanced SearchBrowse

Item

ITEM ACTIONSEXPORT

Released

Conference Paper

Using large eddy simulation to study slope and open-ocean convection in the East/Japan Sea

Authors

Kim,  Bong-Gwan
IUGG 2023, General Assemblies, 1 General, International Union of Geodesy and Geophysics (IUGG), External Organizations;

Cho,  Yang-Ki
IUGG 2023, General Assemblies, 1 General, International Union of Geodesy and Geophysics (IUGG), External Organizations;

Noh,  Yign
IUGG 2023, General Assemblies, 1 General, International Union of Geodesy and Geophysics (IUGG), External Organizations;

External Ressource
No external resources are shared
Fulltext (public)
There are no public fulltexts stored in GFZpublic
Supplementary Material (public)
There is no public supplementary material available
Citation

Kim, B.-G., Cho, Y.-K., Noh, Y. (2023): Using large eddy simulation to study slope and open-ocean convection in the East/Japan Sea, XXVIII General Assembly of the International Union of Geodesy and Geophysics (IUGG) (Berlin 2023).
https://doi.org/10.57757/IUGG23-2277


Cite as: https://gfzpublic.gfz-potsdam.de/pubman/item/item_5018487
Abstract
Bottom- to intermediate-water formations are crucial for meridional circulation and ventilation in the marginal seas as well as global oceans. Observations in the East/Japan Sea (EJS) suggested that open-ocean convection usually occurs south of Vladivostok and that deep convection occasionally occurs along the continental slope, resulting in bottom water formation. Open-ocean and slope convection processes in the EJS were investigated using large-eddy simulation. Slope convection was demonstrated as dense water, formed by strong wintertime cooling in the shelf, flows down along the continental slope as a bottom Ekman current. The properties of the initial dense water were relatively well conserved during slope convection, but they changed rapidly by mixing with the surrounding waters in the open ocean. Accordingly, slope convection penetrated deeper compared to open-ocean convection under the same surface heat flux. Our numerical experiments showed that, under 20 days of 200 W m-2 surface cooling, slope convection reaches depths greater than 2,700 m, whereas open-ocean convection reaches approximately 700 m depth. The results suggest that slope convection is a potential ventilation process for the deep- and bottom-water formations, whereas open-ocean convection contributes to the intermediate- and central-water formations in the EJS. Additional experiments with various topography revealed that the speed of the convective plume was proportional to the slope inclination; the initial properties remained relatively well conserved on a slope of small inclination. The slope convection could be accelerated by a salinity increase in the shelf due to brine rejection from sea-ice formation.