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branches/2011/dev_NEMO_MERGE_2011/DOC/TexFiles/Chapters/Chap_LDF.tex
r3221 r3267 21 21 and for tracers only, eddy induced advection on tracers). These three aspects 22 22 of the lateral diffusion are set through namelist parameters and CPP keys 23 (see the \textit{nam\_traldf} and \textit{nam\_dynldf} below). 23 (see the \textit{nam\_traldf} and \textit{nam\_dynldf} below). Note 24 that this chapter describes the default implementation of iso-neutral 25 tracer mixing, and Griffies's implementation, which is used if 26 \np{traldf\_grif}=true, is described in Appdx\ref{sec:triad} 24 27 25 28 %-----------------------------------nam_traldf - nam_dynldf-------------------------------------------- … … 128 131 $\ $\newline % force a new ligne 129 132 130 A space variation in the eddy coefficient appeals several remarks:133 The following points are relevant when the eddy coefficient varies spatially: 131 134 132 135 (1) the momentum diffusion operator acting along model level surfaces is 133 136 written in terms of curl and divergent components of the horizontal current 134 (see \S\ref{PE_ldf}). Although the eddy coefficient c anbe set to different values135 in these two terms, this option is not available.137 (see \S\ref{PE_ldf}). Although the eddy coefficient could be set to different values 138 in these two terms, this option is not currently available. 136 139 137 140 (2) with an horizontally varying viscosity, the quadratic integral constraints … … 275 278 276 279 \item[$s$- or hybrid $s$-$z$- coordinate : ] in the current release of \NEMO, 277 there is no specific treatment for iso-neutral mixing in the $s$-coordinate. 280 iso-neutral mixing is only employed for $s$-coordinates if the 281 Griffies scheme is used (\np{traldf\_grif}=true; see Appdx \ref{sec:triad}). 278 282 In other words, iso-neutral mixing will only be accurately represented with a 279 283 linear equation of state (\np{nn\_eos}=1 or 2). In the case of a "true" equation … … 332 336 \end{description} 333 337 334 This implementation is a rather old one. It is similar to the one proposed 335 by Cox [1987], except for the background horizontal diffusion. Indeed, 336 the Cox implementation of isopycnal diffusion in GFDL-type models requires 337 a minimum background horizontal diffusion for numerical stability reasons. 338 To overcome this problem, several techniques have been proposed in which 339 the numerical schemes of the ocean model are modified \citep{Weaver_Eby_JPO97, 340 Griffies_al_JPO98}. Here, another strategy has been chosen \citep{Lazar_PhD97}: 341 a local filtering of the iso-neutral slopes (made on 9 grid-points) prevents 342 the development of grid point noise generated by the iso-neutral diffusion 343 operator (Fig.~\ref{Fig_LDF_ZDF1}). This allows an iso-neutral diffusion scheme 344 without additional background horizontal mixing. This technique can be viewed 345 as a diffusion operator that acts along large-scale (2~$\Delta$x) 346 \gmcomment{2deltax doesnt seem very large scale} 347 iso-neutral surfaces. The diapycnal diffusion required for numerical stability is 348 thus minimized and its net effect on the flow is quite small when compared to 349 the effect of an horizontal background mixing. 338 This implementation is a rather old one. It is similar to the one 339 proposed by Cox [1987], except for the background horizontal 340 diffusion. Indeed, the Cox implementation of isopycnal diffusion in 341 GFDL-type models requires a minimum background horizontal diffusion 342 for numerical stability reasons. To overcome this problem, several 343 techniques have been proposed in which the numerical schemes of the 344 ocean model are modified \citep{Weaver_Eby_JPO97, 345 Griffies_al_JPO98}. Griffies's scheme is now available in \NEMO if 346 \np{traldf\_grif\_iso} is set true; see Appdx \ref{sec:triad}. Here, 347 another strategy is presented \citep{Lazar_PhD97}: a local 348 filtering of the iso-neutral slopes (made on 9 grid-points) prevents 349 the development of grid point noise generated by the iso-neutral 350 diffusion operator (Fig.~\ref{Fig_LDF_ZDF1}). This allows an 351 iso-neutral diffusion scheme without additional background horizontal 352 mixing. This technique can be viewed as a diffusion operator that acts 353 along large-scale (2~$\Delta$x) \gmcomment{2deltax doesnt seem very 354 large scale} iso-neutral surfaces. The diapycnal diffusion required 355 for numerical stability is thus minimized and its net effect on the 356 flow is quite small when compared to the effect of an horizontal 357 background mixing. 350 358 351 359 Nevertheless, this iso-neutral operator does not ensure that variance cannot increase,
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