Changeset 6992 for branches/2015/nemo_v3_6_STABLE/DOC/TexFiles/Chapters/Chap_ZDF.tex

Timestamp:

2016-10-05T14:07:19+02:00 (8 years ago)

Author:

nicolasmartin

Message:

Global reorganisation of DOC directory to ensure the export of NEMO Reference Manual both in PDF & HTML

• Move 'Figures' and 'Namelists' from ./TexFiles? to the root, create 'Styles' directory in ./TexFiles? with corresponding files and generate EPS version of all figures
• Fix LaTex? typos, add the possibility to compile each chapter separately with 'subfiles' package and clean the main LaTeX file by creating 'Preamble.tex' & 'Top_Matter.tex' in ./TexFiles?
• Provide LaTeX2HTML.sh script for producing HTML output (LaTeX2HTML tool needed with patch)
• Remove PDF files from versionned files

File:

• branches/2015/nemo_v3_6_STABLE/DOC/TexFiles/Chapters/Chap_ZDF.tex (modified) (9 diffs)

branches/2015/nemo_v3_6_STABLE/DOC/TexFiles/Chapters/Chap_ZDF.tex

@@ +1 @@
+%\documentclass[NEMO_book]{subfiles}
+%\begin{document}
 % ================================================================
 % Chapter  Vertical Ocean Physics (ZDF)
@@ -233 +235 @@
 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>
 \begin{figure}[!t] \begin{center}
-\includegraphics[width=1.00\textwidth]{./TexFiles/Figures/Fig_mixing_length.pdf}
+\includegraphics[width=1.00\textwidth]{Fig_mixing_length}
 \caption{ \label{Fig_mixing_length} 
 Illustration of the mixing length computation. }
@@ -407 +409 @@
 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>
 \begin{figure}[!t]   \begin{center}
-\includegraphics[width=1.00\textwidth]{./TexFiles/Figures/Fig_ZDF_TKE_time_scheme.pdf}
+\includegraphics[width=1.00\textwidth]{Fig_ZDF_TKE_time_scheme}
 \caption{ \label{Fig_TKE_time_scheme} 
 Illustration of the TKE time integration and its links to the momentum and tracer time integration. }
@@ -586 +588 @@
 value near physical boundaries (logarithmic boundary layer law). $C_{\mu}$ and $C_{\mu'}$ 
 are calculated from stability function proposed by \citet{Galperin_al_JAS88}, or by \citet{Kantha_Clayson_1994} 
-or one of the two functions suggested by \citet{Canuto_2001}  (\np{nn\_stab\_func} = 0, 1, 2 or 3, resp.}). 
+or one of the two functions suggested by \citet{Canuto_2001}  (\np{nn\_stab\_func} = 0, 1, 2 or 3, resp.). 
 The value of $C_{0\mu}$ depends of the choice of the stability function.
 
@@ -658 +660 @@
 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>
 \begin{figure}[!htb]    \begin{center}
-\includegraphics[width=0.90\textwidth]{./TexFiles/Figures/Fig_npc.pdf}
+\includegraphics[width=0.90\textwidth]{Fig_npc}
 \caption{  \label{Fig_npc} 
 Example of an unstable density profile treated by the non penetrative 
@@ -814 +816 @@
 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>
 \begin{figure}[!t]   \begin{center}
-\includegraphics[width=0.99\textwidth]{./TexFiles/Figures/Fig_zdfddm.pdf}
+\includegraphics[width=0.99\textwidth]{Fig_zdfddm}
 \caption{  \label{Fig_zdfddm}
 From \citet{Merryfield1999} : (a) Diapycnal diffusivities $A_f^{vT}$ 
@@ -1143 +1145 @@
 baroclinic and barotropic components which is appropriate when using either the
 explicit or filtered surface pressure gradient algorithms (\key{dynspg\_exp} or 
-{\key{dynspg\_flt}). Extra attention is required, however, when using 
+\key{dynspg\_flt}). Extra attention is required, however, when using 
 split-explicit time stepping (\key{dynspg\_ts}). In this case the free surface 
 equation is solved with a small time step \np{rn\_rdt}/\np{nn\_baro}, while the three 
@@ -1258 +1260 @@
 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>
 \begin{figure}[!t]   \begin{center}
-\includegraphics[width=0.90\textwidth]{./TexFiles/Figures/Fig_ZDF_M2_K1_tmx.pdf}
+\includegraphics[width=0.90\textwidth]{Fig_ZDF_M2_K1_tmx}
 \caption{  \label{Fig_ZDF_M2_K1_tmx} 
 (a) M2 and (b) K1 internal wave drag energy from \citet{Carrere_Lyard_GRL03} ($W/m^2$). }
@@ -1369 +1371 @@
 
 
+%\end{document}