Changeset 11151 for NEMO/trunk/doc/latex/NEMO/subfiles/chap_DYN.tex

Timestamp:

2019-06-20T14:59:58+02:00 (5 years ago)

Author:

nicolasmartin

Message:

New version of NEMO_manual.tex
New class scrreport for the document (KOMA-script version of default report)
Foreword is now placed before ToC.
All figures are configured with 1.0\textwidth as default.
For compatibilty, \frontmatter, \mainmatter and \backmatter cmds have been removed and old fonts in LaTeX subfiles have been replaced

• \bf -> \mathbf or \bfseries
• \it -> \itshape
• \rm -> \mathrm or \rmfamily
• \tt -> \ttfamily

File:

• NEMO/trunk/doc/latex/NEMO/subfiles/chap_DYN.tex (modified) (8 diffs)

NEMO/trunk/doc/latex/NEMO/subfiles/chap_DYN.tex

@@ -309 +309 @@
 \begin{figure}[!ht]
   \begin{center}
-    \includegraphics[width=0.70\textwidth]{Fig_DYN_een_triad}
+    \includegraphics[width=\textwidth]{Fig_DYN_een_triad}
     \caption{
       \protect\label{fig:DYN_een_triad}
@@ -862 +862 @@
 \begin{equation}
   \label{eq:BT_dyn}
-  \frac{\partial {\rm \overline{{\bf U}}_h} }{\partial t}=
-  -f\;{\rm {\bf k}}\times {\rm \overline{{\bf U}}_h}
-  -g\nabla _h \eta -\frac{c_b^{\textbf U}}{H+\eta} \rm {\overline{{\bf U}}_h} + \rm {\overline{\bf G}}
+  \frac{\partial {\mathrm \overline{{\mathbf U}}_h} }{\partial t}=
+  -f\;{\mathrm {\mathbf k}}\times {\mathrm \overline{{\mathbf U}}_h}
+  -g\nabla _h \eta -\frac{c_b^{\textbf U}}{H+\eta} \mathrm {\overline{{\mathbf U}}_h} + \mathrm {\overline{\mathbf G}}
 \end{equation}
 \[
   % \label{eq:BT_ssh}
-  \frac{\partial \eta }{\partial t}=-\nabla \cdot \left[ {\left( {H+\eta } \right) \; {\rm{\bf \overline{U}}}_h \,} \right]+P-E
+  \frac{\partial \eta }{\partial t}=-\nabla \cdot \left[ {\left( {H+\eta } \right) \; {\mathrm{\mathbf \overline{U}}}_h \,} \right]+P-E
 \]
 % \end{subequations}
-where $\rm {\overline{\bf G}}$ is a forcing term held constant, containing coupling term between modes,
+where $\mathrm {\overline{\mathbf G}}$ is a forcing term held constant, containing coupling term between modes,
 surface atmospheric forcing as well as slowly varying barotropic terms not explicitly computed to gain efficiency.
 The third term on the right hand side of \autoref{eq:BT_dyn} represents the bottom stress
@@ -884 +884 @@
 \begin{figure}[!t]
   \begin{center}
-    \includegraphics[width=0.7\textwidth]{Fig_DYN_dynspg_ts}
+    \includegraphics[width=\textwidth]{Fig_DYN_dynspg_ts}
     \caption{
       \protect\label{fig:DYN_dynspg_ts}
@@ -1092 +1092 @@
   \[
     % \label{eq:spg_flt}
-    \frac{\partial {\rm {\bf U}}_h }{\partial t}= {\rm {\bf M}}
+    \frac{\partial {\mathrm {\mathbf U}}_h }{\partial t}= {\mathrm {\mathbf M}}
     - g \nabla \left( \tilde{\rho} \ \eta \right)
     - g \ T_c \nabla \left( \widetilde{\rho} \ \partial_t \eta \right)
@@ -1098 +1098 @@
   where $T_c$, is a parameter with dimensions of time which characterizes the force,
   $\widetilde{\rho} = \rho / \rho_o$ is the dimensionless density,
-  and $\rm {\bf M}$ represents the collected contributions of the Coriolis, hydrostatic pressure gradient,
+  and $\mathrm {\mathbf M}$ represents the collected contributions of the Coriolis, hydrostatic pressure gradient,
   non-linear and viscous terms in \autoref{eq:PE_dyn}.
 }   %end gmcomment
@@ -1152 +1152 @@
   \left\{
     \begin{aligned}
-      D_u^{l{\rm {\bf U}}} =\frac{1}{e_{1u} }\delta_{i+1/2} \left[ {A_T^{lm}
+      D_u^{l{\mathrm {\mathbf U}}} =\frac{1}{e_{1u} }\delta_{i+1/2} \left[ {A_T^{lm}
           \;\chi } \right]-\frac{1}{e_{2u} {\kern 1pt}e_{3u} }\delta_j \left[ 
         {A_f^{lm} \;e_{3f} \zeta } \right] \\ \\
-      D_v^{l{\rm {\bf U}}} =\frac{1}{e_{2v} }\delta_{j+1/2} \left[ {A_T^{lm}
+      D_v^{l{\mathrm {\mathbf U}}} =\frac{1}{e_{2v} }\delta_{j+1/2} \left[ {A_T^{lm}
           \;\chi } \right]+\frac{1}{e_{1v} {\kern 1pt}e_{3v} }\delta_i \left[ 
         {A_f^{lm} \;e_{3f} \zeta } \right]
@@ -1494 +1494 @@
 \end{equation}
 
-Note a small tolerance ($\mathrm{rn\_wdmin2}$) has been introduced here {\it [Q: Why is
+Note a small tolerance ($\mathrm{rn\_wdmin2}$) has been introduced here {\itshape [Q: Why is
 this necessary/desirable?]}. Substituting from (\ref{dyn_wd_continuity_coef}) gives an
 expression for the coefficient needed to multiply the outward flux at this cell in order
@@ -1541 +1541 @@
 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>
 \begin{figure}[!ht] \begin{center}
-\includegraphics[width=0.8\textwidth]{Fig_WAD_dynhpg}
+\includegraphics[width=\textwidth]{Fig_WAD_dynhpg}
 \caption{ \label{Fig_WAD_dynhpg}
 Illustrations of the three possible combinations of the logical variables controlling the