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

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

2000] Wirth: Param<strong>et</strong>erization of baroclinic instability<br />

573<br />

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

previously published i<strong>de</strong>alized experiments the dynamics far from the boundary appear to<br />

be compl<strong>et</strong>ely slaved to the boundary conditions. Important quantitiesvary almost linearly<br />

b<strong>et</strong>ween their extremal values at or near the boundary. Using periodic boundary conditions<br />

eliminates this problem compl<strong>et</strong>ely.<br />

A novelty of the present work is that a vari<strong>et</strong>y of experimentsare performed with varying<br />

box-size, strength of forcing and viscous dissipation (mo<strong>de</strong>l <strong>par</strong>am<strong>et</strong>ers) to estimate their<br />

(non-) inuence on large-scale quantities like the diagnosed <strong>par</strong>am<strong>et</strong>ers for large-scale<br />

<strong>par</strong>am<strong>et</strong>erization.It is in<strong>de</strong>ed a crucial point of a large-scale <strong>par</strong>am<strong>et</strong>erization that it should<br />

not, or only very weakly, <strong>de</strong>pend on the above mentioned mo<strong>de</strong>l <strong>par</strong>am<strong>et</strong>ers and this should<br />

be checked whenever a <strong>par</strong>am<strong>et</strong>erization is proposed.<br />

An advantage of testing <strong>par</strong>am<strong>et</strong>erizations of baroclinic instability in a quasigeostrophic<br />

experiment is that in this simplied frame work the <strong>par</strong>am<strong>et</strong>erization of layer<br />

thickness as proposed by Gent and McWilliams (1990) is i<strong>de</strong>ntical to the <strong>par</strong>am<strong>et</strong>erization<br />

of vertical mixing, as favored by Greatbatch and Lamb (1990). This means that the results<br />

presented here apply to the same extent to a whole class of <strong>par</strong>am<strong>et</strong>erizations but also<br />

means that the results presented here can give us no hint to which <strong>par</strong>am<strong>et</strong>erization in this<br />

class is b<strong>et</strong>ter.<br />

A disadvantage of the simplicity is that some of the important questions related to the<br />

<strong>par</strong>am<strong>et</strong>erization of baroclinic instability cannot be addressed in this simplied frame<br />

work. One is the important effect on the long-term tracer dynamics (see e.g. Lee <strong>et</strong> al.,<br />

1997). The d<strong>et</strong>ermination of the vertical <strong>de</strong>pen<strong>de</strong>nce of a <strong>par</strong>am<strong>et</strong>erization would require<br />

more baroclinic mo<strong>de</strong>s. We also neglect in our discussion the important point of the effect<br />

of baroclinic instability on the barotropic mo<strong>de</strong> and the related question of how to<br />

implement vertical boundary conditions. For more d<strong>et</strong>ails on this important point we refer<br />

the rea<strong>de</strong>r to Killworth (2000) and Treguier <strong>et</strong> al. (1997). The latter paper also contains a<br />

d<strong>et</strong>ailed discussion on eddy <strong>par</strong>am<strong>et</strong>erization in quasi-geostrophic mo<strong>de</strong>ls. All the experiments<br />

presented here are restricted to the special case of purely zonal forcing. Thus, we<br />

could not consi<strong>de</strong>r the question of anisotropy of the diagnosed large-scale <strong>par</strong>am<strong>et</strong>ers as<br />

found by Rix and Willebrand (1996).<br />

The next short section is <strong>de</strong>voted to the question of the compatibility b<strong>et</strong>ween the<br />

b-plane approximation and periodic boundary conditions in both horizontal directions. In<br />

Section 3 we present the theor<strong>et</strong>ical <strong>de</strong>scription of our numerical experiment which is<br />

introduced in Section 4. The results are then discussed in Section 5.<br />

2. The periodic b-plane<br />

This section may be skipped by people familiar with simulations on the doubly-periodic<br />

b-plane. We use spatially periodic boundary conditions in both horizontal directions. This<br />

is mathematically consistent with the b-plane approximation, for all evolution and<br />

diagnostic equations (see e.g. Hua <strong>et</strong> al., 1998, for a d<strong>et</strong>ailed discussion of this point).<br />

A more subtle point, however, is the validity of the b-plane approximation in a domain<br />

having innite extension in the meridional direction. The quasi-geostrophic potential

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