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Etudes et évaluation de processus océaniques par des hiérarchies ...

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88 CHAPITRE 4. ETUDES DE PROCESSUS OCÉANOGRAPHIQUES<br />

0.006<br />

A. Wirth / Ocean Mo<strong>de</strong>lling 9 (2005) 71–87 85<br />

U (m/s)<br />

0.004<br />

0.002<br />

0<br />

8<br />

16<br />

32<br />

64<br />

128<br />

256<br />

256 long<br />

512<br />

-0.002<br />

-0.004<br />

850 900 950 1000<br />

Depth (m)<br />

Fig. 9. Horizontal velocity along x ¼ 250 m near the lower boundary. Symbols correspond to the different spatial<br />

resolution (as given in the figure).<br />

tel-00545911, version 1 - 13 Dec 2010<br />

W (m/s)<br />

0.003<br />

0.002<br />

0.001<br />

0<br />

-0.001<br />

-0.002<br />

850 900 950 1000<br />

Depth (m)<br />

Fig. 10. Vertical velocity along x ¼ 500 m near the lower boundary. Symbols correspond to the different spatial resolution<br />

(as given in the figure).<br />

No spectral convergence is observed in this test-case. This comes at no surprise as the dynamics<br />

even in the interior of the domain is compl<strong>et</strong>ely slaved to the dynamics at the boundaries and thus<br />

shows the corresponding convergence properties. It is in<strong>de</strong>ed clearly visible from Fig. 7 that no<br />

structures smaller than the basin scale appear in the problem. A problem involving scales smaller<br />

than those imposed by the boundaries would cease to be stationary and the here presented<br />

analysis could not be performed.<br />

With the insight obtained from boundary-layer theory, the velocity components in the buffer<br />

zone can be adjusted so that the real dynamics at the boundary is mo<strong>de</strong>led to higher or<strong>de</strong>r. The<br />

convergence properties of the dynamics in the interior fluid would then follow. This is the subject<br />

of future research.<br />

8<br />

16<br />

32<br />

64<br />

128<br />

256<br />

256 long<br />

512

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