Thursday, 12 June 2008: 10:30 AM
Aula Magna Höger (Aula Magna)
The energy exchange between ocean and atmosphere in the Arctic and Antarctic marginal sea-ice zone is strongly influenced by the extent of sea-ice cover. While ice sheets have an isolating effect, areas with open water or thin new ice generate strong convection and turbulence due to the large temperature difference between air and water, especially in winter. This implies large vertical heat fluxes which significantly modify the structure of the polar atmospheric boundary layer. Open water areas in the sea-ice zone are called leads and polynyas respectively. Polynyas are large open water areas with diameters up to 200 km and more. In contrast to the lake-like polynyas, leads resemble channels in the sea-ice and have a width of several meters up to several kilometers. As leads and polynyas are observed during the whole year in the entire sea-ice zone, they have a significant effect on the polar climate which is still insufficiently considered in weather and climate models. To gain a better understanding of the still not well understood effects of leads on the boundary layer turbulence and to clarify their importance for the energy budget and structure of the ABL, high-resolution large-eddy simulations are performed with the parallelized LES model PALM. The results will later be used to (further) develop parameterizations of the lead effect which can be used in non-eddy resolving models with different grid sizes.
Presented are high-resolution LES results from parameter studies of Antarctic leads concerning different lead sizes, horizontal wind speeds and thermal stratifications. In addition, results of a sensitivity study are shown, in which the grid size is gradually decreased from 2 to 0.25 m. With a resolution of 0.5 m and less it is now possible to resolve turbulence not only behind but also directly above the lead where the height of the convective boundary layer is only a few meters. Furthermore a turbulent inflow is realized, ensuring that the flow is already turbulent when approaching the upstream edge of the lead. Thus, convection starts at a much closer distance downstream of the upstream edge compared to earlier simulations.
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