Update file chap_DYN.tex

latex/NEMO/subfiles/chap_DYN.tex

@@ -675,7 +675,7 @@ cells’ centre. This scheme works well for moderately steep computational level
 when model levels are steeply inclined. 
 
 \item
-\textbf{Density Jacobian with cubic polynomial scheme} (\np[=.true.]{ln_hpg_djc}{ln\_hpg\_djc}, \cite{shchepetkin.mcwilliams_jgro03}:
+\textbf{Density Jacobian with cubic polynomial scheme} (\np[=.true.]{ln_hpg_djc}{ln\_hpg\_djc}, \cite{shchepetkin.mcwilliams_jgro03}):
 
 the ROMS-like, density Jacobian with cubic polynomial method has been debugged and from vn4.2 is available as an option. 
 This scheme is based on section 5 of \cite{shchepetkin.mcwilliams_jgro03} For the force in the $i$-direction, it uses constrained cubic 
@@ -846,7 +846,7 @@ no slip or partial slip boundary conditions are applied according to the user's
 \subsection[Iso-level laplacian (\forcode{ln_dynldf_lap})]{Iso-level laplacian operator (\protect\np{ln_dynldf_lap}{ln\_dynldf\_lap})}
 \label{subsec:DYN_ldf_lap}
 
-For lateral iso-level diffusion, the discrete operator is:
+For lateral iso-level diffusion (\np[=0]{nn_dynldf_typ}{nn\_dynldf\_typ}), the discrete operator is:
 \begin{equation}
   \label{eq:DYN_ldf_lap}
   \left\{
@@ -864,7 +864,7 @@ For lateral iso-level diffusion, the discrete operator is:
 As explained in \autoref{sec:DIFFOPERS_3}, this formulation (as the gradient of a divergence and curl of the vorticity) preserves 
 symmetry and ensures a complete separation between the vorticity and divergence parts of the momentum diffusion.
 
-In v5.0 a symetrical lateral iso-level operator has been introduced : 
+In v5.0 a symetrical lateral iso-level operator (\np[=1]{nn_dynldf_typ}{nn\_dynldf\_typ}) has been introduced : 
 \begin{equation}
   \label{eq:DYN_ldf_lap_sym}
   \left\{