02.02.2013 Views

D28: Internal seiche mixing study - Hydromod

D28: Internal seiche mixing study - Hydromod

D28: Internal seiche mixing study - Hydromod

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Integrated Water Resource Management for Important Deep European Lakes and their Catchment Areas<br />

EUROLAKES<br />

<strong>D28</strong>: <strong>Internal</strong> <strong>seiche</strong> <strong>mixing</strong> <strong>study</strong><br />

FP5_Contract No.: EVK1-CT1999-00004<br />

Version: 1.2<br />

Date: 24.08.2004<br />

File: <strong>D28</strong>.doc<br />

Page 76 of 92<br />

from another location, tells the following example. Take the initial information at the<br />

central position of Lake Überlingen, where amplitudes of about 12 m are of common<br />

occurrence (Bäuerle et al., 1998): From Figure 44 it is inferred that at central Lake<br />

Überlingen the amplitude of the interface displacement is about 90 % of the maximum.<br />

This in turn yields that 13.3 m is the corresponding amplitude at the very end of Lake<br />

Überlingen. Finally, in analogy to the above case of reference, we get<br />

13.3 x 4300/1500 = 38 cm/s and 13.3 x 4300/8500 = 6.7 cm/s as vertically averaged<br />

velocities in the upper and lower layer in the Straits of Mainau, respectively, which correspond<br />

to an amplitude of 12 m measured at a central position of Lake Überlingen.<br />

Figure 52 : Current field of the eleventh internal mode in the surface-layer on 13 April 1989 with<br />

T11 = 39.8 h. The normalised maximum transport occurs at the mouth of the Bay of Constance and<br />

amounts to about 5600 cm²/s. The cross mark near the southern shore in the eastern half of the<br />

lake designates the site of the waste water intake discussed in the text. (further explanation in<br />

Figure 50)<br />

It should be mentioned that the same value of the phase velocity of long internal waves<br />

ci results from different combinations of he and ε according to the relations (1), (2), (8).<br />

Since the eigen-solutions of the problem (5) are uniquely determined for a very phase<br />

speed, ci, the respective definite transport field of the mode in question has to be<br />

evaluated with regard to he, i.e. the associated combination of h1 and h2, which fit together<br />

with ε in the relation (8). In this sense, there is a certain variety of two-layer<br />

manifestations equivalently related to a unique set of eigen-solutions. Thus, for the<br />

same maximum amplitude of a mode of them different definite transports result at a<br />

selected place, just depending on the differences allowed for by both the associated

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!