Changeset 996 for trunk/DOC/TexFiles/Chapters/Chap_LDF.tex

Timestamp:

2008-05-28T12:38:21+02:00 (16 years ago)

Author:

gm

Message:

trunk - DOC update to correct error in previous update

File:

• trunk/DOC/TexFiles/Chapters/Chap_LDF.tex (modified) (1 diff)

trunk/DOC/TexFiles/Chapters/Chap_LDF.tex

@@ -9 +9 @@
 $\ $\newline    % force a new ligne
 
-The lateral physics on momentum and tracer equations have been given in \S\ref{PE_zdf} and their discrete formulation in \S\ref{TRA_ldf} and \S\ref{DYN_ldf}). In this section we 
-further discuss the choices that underlie each lateral physics option. 
-Choosing one lateral physics means for the user defining, (1) the space and time variations of the eddy coefficients ; (2) the direction along which the lateral diffusive fluxes are evaluated (model level, geopotential or isopycnal surfaces); and (3) the type of operator used (harmonic, or biharmonic operators, and for tracers only, eddy induced advection on tracers). These 
-three aspects of the lateral diffusion are set through namelist parameters and CPP keys (see the nam\_traldf and nam\_dynldf below).
+The lateral physics on momentum and tracer equations have been given in 
+\S\ref{PE_zdf} and their discrete formulation in \S\ref{TRA_ldf} and \S\ref{DYN_ldf}). 
+In this section we further discuss the choices that underlie each lateral physics option. 
+Choosing one lateral physics means for the user defining, (1) the space and time 
+variations of the eddy coefficients ; (2) the direction along which the lateral diffusive 
+fluxes are evaluated (model level, geopotential or isopycnal surfaces); and (3) the 
+type of operator used (harmonic, or biharmonic operators, and for tracers only, eddy 
+induced advection on tracers). These three aspects of the lateral diffusion are set 
+through namelist parameters and CPP keys (see the nam\_traldf and nam\_dynldf 
+below).
 %-----------------------------------nam_traldf - nam_dynldf--------------------------------------------
 \namdisplay{nam_traldf}