This builds locally (updates to chap_DYN.tex). Also updated namelist submodule

latex/NEMO/subfiles/chap_DYN.tex

@@ -161,7 +161,7 @@ This option can be useful when the value of the timestep is limited by vertical
 \end{listing}
 
 The vector invariant form of the momentum equation is most commonly used in
-coarse-resolution applications of the \NEMO\ ocean model.  For higher resolutions it
+coarse-resolution (1$^\textrm{o}$) applications of the \NEMO\ ocean model.  For higher resolutions it
 requires the activation of Hollingsworth correction (\np[=1]{nn_dynkeg}{nn\_dynkeg})
 following Arakawa (2001) The flux form option (see next section) has been present since
 version $2$.  By structuring the equations in vector invariant form, the dynamics are
@@ -412,12 +412,14 @@ no slip or partial slip boundary conditions are applied following \autoref{chap:
 In flux form, the vorticity term reduces to a Coriolis term in which the Coriolis parameter has been modified to account for the "metric" term.
 This altered Coriolis parameter is thus discretised at $f$-points.
 It is given by:
-\begin{aligned*}
+\[
+\begin{aligned}
   % \label{eq:DYN_cor_metric}
   f+\frac{1}{e_1 e_2 }\left( {v\frac{\partial e_2 }{\partial i}  -  u\frac{\partial e_1 }{\partial j}} \right)
   \equiv   f + \frac{1}{e_{1f} e_{2f} } \left( \overline v ^{i+1/2}\delta_{i+1/2} \left[ {e_{2u} } \right]
       -  \overline u ^{j+1/2}\delta_{j+1/2} \left[ {e_{1u} } \right] \right)
-\end{aligned*}
+\end{aligned}
+\]
 
 %                 energy conserving scheme at T-point
 %% =================================================================================================
@@ -457,21 +459,21 @@ it is is centred in time (\textit{now} velocity) at stage 2 and 3.
 \label{subsec:DYN_adv_flux}
 
 The discrete expression of the advection term is given by:
-\[
+\begin{equation}
   % \label{eq:DYN_adv}
   \left\{
     \begin{aligned}
       \frac{1}{e_{1u}\,e_{2u}\,e_{3u}} 
-      \left( \delta_{i+1/2} \left[ \overline{e_{2u}\,e_{3u}\;u }^{i} \ u_t \right]
-        + & \delta_{j} \left[ \overline{e_{1u}\,e_{3u}\;v }^{i+1/2} \ u_f \right] \right.  \\
-       \left. + & \delta_{k} \left[ \overline{e_{1w}\,e_{2w}\;w}^{i+1/2} \ u_{uw} \right] \right)   \\[10pt]
+      \left( \delta_{i+1/2} \left[ \overline{e_{2u}\,e_{3u}\;u }^{i} \ u_t \right] \right.
+        + & \delta_{j} \left[ \overline{e_{1u}\,e_{3u}\;v }^{i+1/2} \ u_f \right]  \\
+        + & \left. \delta_{k} \left[ \overline{e_{1w}\,e_{2w}\;w}^{i+1/2} \ u_{uw} \right] \right)   \\[10pt]
       \frac{1}{e_{1v}\,e_{2v}\,e_{3v}}
-      \left( \delta_{i} \left[ \overline{e_{2u}\,e_{3u }\;u }^{j+1/2} \ v_f \right]
-        + & \delta_{j+1/2} \left[ \overline{e_{1u}\,e_{3u }\;v }^{i} \ v_t \right] \right.  \\
-       \left. + & \delta_{k} \left[ \overline{e_{1w}\,e_{2w}\;w}^{j+1/2} \ v_{vw} \right] \right) \\
+      \left( \delta_{i} \left[ \overline{e_{2u}\,e_{3u }\;u }^{j+1/2} \ v_f \right] \right.
+        + & \delta_{j+1/2} \left[ \overline{e_{1u}\,e_{3u }\;v }^{i} \ v_t \right]  \\
+        + & \left. \delta_{k} \left[ \overline{e_{1w}\,e_{2w}\;w}^{j+1/2} \ v_{vw} \right] \right) \\
     \end{aligned}
   \right.
-\]
+\end{equation}
 
 Two advection schemes are available:
 a $2^{nd}$ order centered finite difference scheme, CEN2,

namelists @ 10fd1134

-Subproject commit 43a9e90e73133b4d705f0576a474c5c0b04c2204
+Subproject commit 10fd1134aba6ea0c748fbd47cc95a9172ac6b838