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Changeset 11598 for NEMO/trunk/doc/latex/NEMO/subfiles/chap_DYN.tex – NEMO

Ignore:
Timestamp:
2019-09-25T22:00:42+02:00 (5 years ago)
Author:
nicolasmartin
Message:

Add template of versioning record at the beginning of chapters

File:
1 edited

Legend:

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

    r11597 r11598  
    22 
    33\begin{document} 
     4 
    45\chapter{Ocean Dynamics (DYN)} 
    56\label{chap:DYN} 
    67 
     8\thispagestyle{plain} 
     9 
    710\chaptertoc 
     11 
     12\paragraph{Changes record} ~\\ 
     13 
     14{\footnotesize 
     15  \begin{tabularx}{\textwidth}{l||X|X} 
     16    Release & Author(s) & Modifications \\ 
     17    \hline 
     18    {\em   4.0} & {\em ...} & {\em ...} \\ 
     19    {\em   3.6} & {\em ...} & {\em ...} \\ 
     20    {\em   3.4} & {\em ...} & {\em ...} \\ 
     21    {\em <=3.4} & {\em ...} & {\em ...} 
     22  \end{tabularx} 
     23} 
     24 
     25\clearpage 
    826 
    927Using the representation described in \autoref{chap:DOM}, 
     
    149167(see \autoref{subsec:DOM_Num_Index_vertical}). 
    150168 
    151  
    152169%% ================================================================================================= 
    153170\section{Coriolis and advection: vector invariant form} 
     
    301318  \label{fig:DYN_een_triad} 
    302319\end{figure} 
    303 % >>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>> 
    304320 
    305321A key point in \autoref{eq:DYN_een_e3f} is how the averaging in the \textbf{i}- and \textbf{j}- directions is made. 
     
    387403a similar split-explicit time stepping should be used on vertical advection of tracer to ensure a better stability, 
    388404an option which is only available with a TVD scheme (see \np{ln_traadv_tvd_zts}{ln\_traadv\_tvd\_zts} in \autoref{subsec:TRA_adv_tvd}). 
    389  
    390405 
    391406%% ================================================================================================= 
     
    834849(see their figure 12, lower left). 
    835850 
    836 %>   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   > 
    837851\begin{figure}[!t] 
    838852  \centering 
     
    859873  \label{fig:DYN_spg_ts} 
    860874\end{figure} 
    861 %>   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   >   > 
    862875 
    863876In the default case (\np[=.true.]{ln_bt_fw}{ln\_bt\_fw}), 
     
    909922it is still significant as shown by \citet{levier.treguier.ea_rpt07} in the case of an analytical barotropic Kelvin wave. 
    910923 
    911 %>>>>>=============== 
    912924\gmcomment{               %%% copy from griffies Book 
    913925 
     
    10281040 
    10291041}            %%end gm comment (copy of griffies book) 
    1030  
    1031 %>>>>>=============== 
    10321042 
    10331043%% ================================================================================================= 
     
    12511261the snow-ice mass is taken into account when computing the surface pressure gradient. 
    12521262 
    1253  
    12541263\gmcomment{ missing : the lateral boundary condition !!!   another external forcing 
    12551264 } 
     
    13071316The final sub-section covers some additional considerations that are relevant to both schemes. 
    13081317 
    1309  
    13101318%   Iterative limiters 
    13111319%% ================================================================================================= 
     
    13361344to be its depth times its velocity. This depth is considered to be zero at ``dry'' $u$-points consistent with its 
    13371345treatment in the calculation of the flux of mass across the cell face. 
    1338  
    13391346 
    13401347\cite{warner.defne.ea_CG13} state that in their scheme the velocity masks at the cell faces for the baroclinic 
     
    14621469directional limiter does. 
    14631470 
    1464  
    14651471%      Surface pressure gradients 
    14661472%% ================================================================================================= 
     
    14811487column.  The three possible combinations are illustrated in \autoref{fig:DYN_WAD_dynhpg}. 
    14821488 
    1483 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>> 
    14841489\begin{figure}[!ht] 
    14851490  \centering 
     
    14911496  \label{fig:DYN_WAD_dynhpg} 
    14921497\end{figure} 
    1493 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>> 
    14941498 
    14951499The first logical, $\mathrm{ll\_tmp1}$, is set to true if and only if the water depth at 
     
    15541558See the WAD tests MY\_DOC documention for details of the WAD test cases. 
    15551559 
    1556  
    1557  
    15581560%% ================================================================================================= 
    15591561\section[Time evolution term (\textit{dynnxt.F90})]{Time evolution term (\protect\mdl{dynnxt})} 
    15601562\label{sec:DYN_nxt} 
    1561  
    15621563 
    15631564Options are defined through the \nam{dom}{dom} namelist variables. 
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