Changeset 2349 for branches/nemo_v3_3_beta/DOC/TexFiles/Chapters/Chap_LDF.tex

Timestamp:

2010-11-01T15:21:01+01:00 (13 years ago)

Author:

gm

Message:

v3.3beta: #658 phasing of the doc - key check + many minor changes

File:

• branches/nemo_v3_3_beta/DOC/TexFiles/Chapters/Chap_LDF.tex (modified) (5 diffs)

branches/nemo_v3_3_beta/DOC/TexFiles/Chapters/Chap_LDF.tex

@@ -57 +57 @@
 The specification of the space variation of the coefficient is made in 
 \mdl{ldftra} and \mdl{ldfdyn}, or more precisely in include files 
-\textit{ldftra\_cNd.h90} and \textit{ldfdyn\_cNd.h90}, with N=1, 2 or 3. 
+\textit{traldf\_cNd.h90} and \textit{dynldf\_cNd.h90}, with N=1, 2 or 3. 
 The user can modify these include files as he/she wishes. The way the 
 mixing coefficient are set in the reference version can be briefly described 
@@ -63 +63 @@
 
 \subsubsection{Constant Mixing Coefficients (default option)}
-When none of the \textbf{key\_ldfdyn\_...} and \textbf{key\_ldftra\_...} keys are 
+When none of the \textbf{key\_dynldf\_...} and \textbf{key\_traldf\_...} keys are 
 defined, a constant value is used over the whole ocean for momentum and 
 tracers, which is specified through the \np{rn\_ahm0} and \np{rn\_aht0} namelist 
 parameters.
 
-\subsubsection{Vertically varying Mixing Coefficients (\key{ldftra\_c1d} and \key{ldfdyn\_c1d})} 
+\subsubsection{Vertically varying Mixing Coefficients (\key{traldf\_c1d} and \key{dynldf\_c1d})} 
 The 1D option is only available when using the $z$-coordinate with full step. 
 Indeed in all the other types of vertical coordinate, the depth is a 3D function 
@@ -77 +77 @@
 and the transition takes place around z=300~m with a width of 300~m 
 ($i.e.$ both the depth and the width of the inflection point are set to 300~m). 
-This profile is hard coded in file \hf{ldftra\_c1d}, but can be easily modified by users.
-
-\subsubsection{Horizontally Varying Mixing Coefficients (\key{ldftra\_c2d} and \key{ldfdyn\_c2d})}
+This profile is hard coded in file \hf{traldf\_c1d}, but can be easily modified by users.
+
+\subsubsection{Horizontally Varying Mixing Coefficients (\key{traldf\_c2d} and \key{dynldf\_c2d})}
 By default the horizontal variation of the eddy coefficient depends on the local mesh 
 size and the type of operator used:
@@ -110 +110 @@
 defined, see \hf{ldfdyn\_antarctic} and \hf{ldfdyn\_arctic}).
 
-\subsubsection{Space Varying Mixing Coefficients (\key{ldftra\_c3d} and \key{ldfdyn\_c3d})}
+\subsubsection{Space Varying Mixing Coefficients (\key{traldf\_c3d} and \key{dynldf\_c3d})}
 
 The 3D space variation of the mixing coefficient is simply the combination of the 
@@ -148 +148 @@
 spurious diapycnal diffusion (see {\S\ref{LDF_slp}).
 
-(4) when an eddy induced advection term is used (\key{trahdf\_eiv}), $A^{eiv}$, 
+(4) when an eddy induced advection term is used (\key{traldf\_eiv}), $A^{eiv}$, 
 the eddy induced coefficient has to be defined. Its space variations are controlled 
 by the same CPP variable as for the eddy diffusivity coefficient ($i.e.$