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Baltic Sea

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Figure 1.2: Bathymetric map of the Eastern Gotland Basin (blue square in Fig. 1.1) with positions of<br />

the mooring sites northeast (NE) and south-west (SW) deployed 1997-98, the central <strong>Baltic</strong> monitoring<br />

station BMP271 of the HELCOM programme (star) and hydrographic stations of the MESODYN M-<br />

7 (13×16 stations) and M-8 (13×15 stations) campaigns (small dots). The horizontal line marks the<br />

position of the vertical sections in Fig. 3.5. Note the 170 m isoline bounds the enclosed parts of the deep<br />

basin.<br />

terminated by a substantial inow event observed in 1993. It was the objective of a number<br />

of investigations. Changes in meso-scale thermohaline variability and driving mechanisms of<br />

intrusions as a result of this inow were analysed on the base of eld observations as well<br />

as by scenarios simulated by hydrographic circulation models, Zhurbas and Paka (1997),<br />

Zhurbas and Paka (1999), Zhurbas et al. (2003) and Kuzmina et al. (2005).<br />

Zhurbas and Paka (1997) and Zhurbas and Paka (1999) used closely spaced CTD<br />

proles ranging from the Stolpe Channel to the Gotland Basin three months after the 1993<br />

inow to also investigate intrusive layering and its most important features. Thus, these<br />

authors presented results which describe several consequences of such deep water intrusions,<br />

especially with respect to the generation of eddy-like features on the meso-scale. Kuzmina<br />

et al. (2005) also studied associated driving mechanisms and concluded that embedded<br />

diusive convection also works in the <strong>Baltic</strong> halocline. It triggers diapycnal mixing, regardless<br />

of the overwhelming stratication. Due to the observed homogenisation of the deep water,<br />

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