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

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

A. Wirth <strong>et</strong> al. / Deep-Sea Research II 49 (2002) 1279–1295 1293<br />

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

Fig. 10. Mean layer thickness vs. meridional position of the GW in the different experiments with the RG mo<strong>de</strong>l. Triangles, squares<br />

and circles correspond to exps. with forcings of the years 1993, 1995 and 1996, respectively; solid and open symbols are for low and<br />

high-friction experiments, respectively; large symbols represent the mean values.<br />

August, the circulation in the western Arabian Sea<br />

is strongly influenced by turbulent (mostly anticyclonic)<br />

eddies. Consequently, from September<br />

on the GW is characterized by chaotic dynamics<br />

rather than a regular life cycle.<br />

We have <strong>de</strong>monstrated that the year-to-year<br />

variability of ocean currents in the western<br />

Arabian Sea is not only influenced by variability<br />

in the wind forcing but is substantially influenced<br />

by internally generated variability. This latter<br />

variability has a white spectrum on interannual<br />

time scales, and a prediction of the internally<br />

caused variability seems impossible on time scales<br />

longer than a month.<br />

A critical <strong>par</strong>am<strong>et</strong>er in the RG mo<strong>de</strong>l is<br />

dissipation values that have been chosen here for<br />

reasons of numerical stability and smoothness.<br />

This choice, while common, is not based on<br />

physical consi<strong>de</strong>rations, and an uncomfortable<br />

conclusion is that the mo<strong>de</strong>l results <strong>de</strong>pend on<br />

the value of that <strong>par</strong>am<strong>et</strong>er. Preliminary experiments<br />

with a friction coefficient of 0:3 <br />

10 3 m 2 s 1 suggest that the variability of largescale<br />

quantities still increases with <strong>de</strong>creasing<br />

friction.<br />

As remarked above, Exp. PE-lo can be consi<strong>de</strong>red<br />

as the most realistic of all runs and can best<br />

be com<strong>par</strong>ed with observations. For the interpr<strong>et</strong>ation<br />

of such a com<strong>par</strong>ison, it would be<br />

necessary to assess the internal variability in that<br />

mo<strong>de</strong>l. If the differences in GW position as shown<br />

in Table 2 were indicative of the overall dissipation,<br />

it would follow that the internal variability in<br />

PE-lo were higher than in any of the RG mo<strong>de</strong>ls.<br />

From our experiments we have, however, no direct<br />

estimate of the internal <strong>par</strong>t of the variability in<br />

either of the PE mo<strong>de</strong>ls, due to the prohibitive<br />

computational expenses.<br />

In summary, our findings suggest that internal<br />

variability is so high that a direct com<strong>par</strong>ison<br />

b<strong>et</strong>ween observations and eddy-resolving mo<strong>de</strong>ls<br />

of large-scale quantities like the GW is only<br />

meaningful if an ensemble of mo<strong>de</strong>l experiments<br />

is consi<strong>de</strong>red. A com<strong>par</strong>ison of actual mo<strong>de</strong>l<br />

realizations to observations would be meaningful<br />

only in the context of data assimilation where the

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