Changeset 11598 for NEMO/trunk/doc/latex/NEMO/subfiles/chap_DYN.tex
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- 2019-09-25T22:00:42+02:00 (5 years ago)
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NEMO/trunk/doc/latex/NEMO/subfiles/chap_DYN.tex
r11597 r11598 2 2 3 3 \begin{document} 4 4 5 \chapter{Ocean Dynamics (DYN)} 5 6 \label{chap:DYN} 6 7 8 \thispagestyle{plain} 9 7 10 \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 8 26 9 27 Using the representation described in \autoref{chap:DOM}, … … 149 167 (see \autoref{subsec:DOM_Num_Index_vertical}). 150 168 151 152 169 %% ================================================================================================= 153 170 \section{Coriolis and advection: vector invariant form} … … 301 318 \label{fig:DYN_een_triad} 302 319 \end{figure} 303 % >>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>304 320 305 321 A key point in \autoref{eq:DYN_een_e3f} is how the averaging in the \textbf{i}- and \textbf{j}- directions is made. … … 387 403 a similar split-explicit time stepping should be used on vertical advection of tracer to ensure a better stability, 388 404 an 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}). 389 390 405 391 406 %% ================================================================================================= … … 834 849 (see their figure 12, lower left). 835 850 836 %> > > > > > > > > > > > > > > > > > > > > > > > > > > >837 851 \begin{figure}[!t] 838 852 \centering … … 859 873 \label{fig:DYN_spg_ts} 860 874 \end{figure} 861 %> > > > > > > > > > > > > > > > > > > > > > > > > > > >862 875 863 876 In the default case (\np[=.true.]{ln_bt_fw}{ln\_bt\_fw}), … … 909 922 it is still significant as shown by \citet{levier.treguier.ea_rpt07} in the case of an analytical barotropic Kelvin wave. 910 923 911 %>>>>>===============912 924 \gmcomment{ %%% copy from griffies Book 913 925 … … 1028 1040 1029 1041 } %%end gm comment (copy of griffies book) 1030 1031 %>>>>>===============1032 1042 1033 1043 %% ================================================================================================= … … 1251 1261 the snow-ice mass is taken into account when computing the surface pressure gradient. 1252 1262 1253 1254 1263 \gmcomment{ missing : the lateral boundary condition !!! another external forcing 1255 1264 } … … 1307 1316 The final sub-section covers some additional considerations that are relevant to both schemes. 1308 1317 1309 1310 1318 % Iterative limiters 1311 1319 %% ================================================================================================= … … 1336 1344 to be its depth times its velocity. This depth is considered to be zero at ``dry'' $u$-points consistent with its 1337 1345 treatment in the calculation of the flux of mass across the cell face. 1338 1339 1346 1340 1347 \cite{warner.defne.ea_CG13} state that in their scheme the velocity masks at the cell faces for the baroclinic … … 1462 1469 directional limiter does. 1463 1470 1464 1465 1471 % Surface pressure gradients 1466 1472 %% ================================================================================================= … … 1481 1487 column. The three possible combinations are illustrated in \autoref{fig:DYN_WAD_dynhpg}. 1482 1488 1483 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>1484 1489 \begin{figure}[!ht] 1485 1490 \centering … … 1491 1496 \label{fig:DYN_WAD_dynhpg} 1492 1497 \end{figure} 1493 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>1494 1498 1495 1499 The first logical, $\mathrm{ll\_tmp1}$, is set to true if and only if the water depth at … … 1554 1558 See the WAD tests MY\_DOC documention for details of the WAD test cases. 1555 1559 1556 1557 1558 1560 %% ================================================================================================= 1559 1561 \section[Time evolution term (\textit{dynnxt.F90})]{Time evolution term (\protect\mdl{dynnxt})} 1560 1562 \label{sec:DYN_nxt} 1561 1562 1563 1563 1564 Options are defined through the \nam{dom}{dom} namelist variables.
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