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Date 31.8.1997, 03.11.1997, 03.11.1997, 17.2.1998, 17.2.1998, 18.2.1998, 27.3.1998, 21.4.1998,<br />

UTC 21:12h 07:31h 08:52h 18:07h 20:49h 07:09h 01:20h 14:57h<br />

〈R ρ〉 0.044 0.060 0.059 0.220 0.221 0.238 0.164 0.184<br />

Std Dev 〈R ρ〉 1.219 0.032 0.035 0.133 0.165 0.116 0.458 0.090<br />

〈T u〉 −47.49 −48.45 −48.39 −57.38 −57.44 −58.39 −54.30 −54.45<br />

Table 3.2: Vertical averaged density ratio 〈R ρ 〉 with the standard deviation (Std Dev) and vertically<br />

averaged Turner angles 〈Tu〉 of BMP271 between 170- 235 m for proles shown in Fig. 3.8.<br />

Figure 3.9: Sketch of salinity/ heat budget calculations in the EGB for proles in shown Fig. 3.10.<br />

that diusive convection essentially controls the diapycnal mixing within intermediate layers<br />

(90-170 m), especially in the wake of deep warm-water intrusions reaching the EGB.<br />

3.2.4 Salinity and heat budgets<br />

Estimates for the eective diusivities in the deepest layers of the EGB may be obtained from<br />

basin-scale scalar budgets as suggested e.g. for the <strong>Baltic</strong> <strong>Sea</strong> by Stigebrandt (1987) and<br />

Axell (1998), as well as for some semi-enclosed deep basins o the Californian coast by<br />

Ledwell and Hickey (1995).<br />

Here, the starting point is selected to be the salinity budget for a xed control volume, V ,<br />

underneath a level surface, A t , located at the vertical position z = z t ,<br />

d<br />

dt<br />

∫<br />

V<br />

∫<br />

∫<br />

S dV = − Sw dA −<br />

A t<br />

A t<br />

F S dA , (3.3)<br />

where w and F S denote the vertical (upward) components of the velocity and the turbulent<br />

salt ux, respectively. The only assumption involved in the derivation of (3.3) is the absence of<br />

37

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