Changeset 11558 for NEMO/trunk/doc/latex/NEMO/subfiles/chap_DYN.tex
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- 2019-09-17T17:04:06+02:00 (5 years ago)
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NEMO/trunk/doc/latex/NEMO/subfiles/chap_DYN.tex
r11552 r11558 166 166 %-----------------------------------------nam_dynadv---------------------------------------------------- 167 167 168 \nlst{namdyn_adv} 168 \begin{listing} 169 \nlst{namdyn_adv} 170 \caption{\texttt{namdyn\_adv}} 171 \label{lst:namdyn_adv} 172 \end{listing} 169 173 %------------------------------------------------------------------------------------------------------------- 170 174 … … 185 189 %------------------------------------------nam_dynvor---------------------------------------------------- 186 190 187 \nlst{namdyn_vor} 191 \begin{listing} 192 \nlst{namdyn_vor} 193 \caption{\texttt{namdyn\_vor}} 194 \label{lst:namdyn_vor} 195 \end{listing} 188 196 %------------------------------------------------------------------------------------------------------------- 189 197 … … 308 316 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>> 309 317 \begin{figure}[!ht] 310 \begin{center} 311 \includegraphics[width=\textwidth]{Fig_DYN_een_triad} 312 \caption{ 313 \protect\label{fig:DYN_een_triad} 314 Triads used in the energy and enstrophy conserving scheme (een) for 315 $u$-component (upper panel) and $v$-component (lower panel). 316 } 317 \end{center} 318 \centering 319 \includegraphics[width=\textwidth]{Fig_DYN_een_triad} 320 \caption[Triads used in the energy and enstrophy conserving scheme (EEN)]{ 321 Triads used in the energy and enstrophy conserving scheme (EEN) for 322 $u$-component (upper panel) and $v$-component (lower panel).} 323 \label{fig:DYN_een_triad} 318 324 \end{figure} 319 325 % >>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>> … … 416 422 %------------------------------------------nam_dynadv---------------------------------------------------- 417 423 418 \nlst{namdyn_adv}419 424 %------------------------------------------------------------------------------------------------------------- 420 425 … … 564 569 %------------------------------------------nam_dynhpg--------------------------------------------------- 565 570 566 \nlst{namdyn_hpg} 571 \begin{listing} 572 \nlst{namdyn_hpg} 573 \caption{\texttt{namdyn\_hpg}} 574 \label{lst:namdyn_hpg} 575 \end{listing} 567 576 %------------------------------------------------------------------------------------------------------------- 568 577 … … 778 787 %-----------------------------------------nam_dynspg---------------------------------------------------- 779 788 780 \nlst{namdyn_spg} 789 \begin{listing} 790 \nlst{namdyn_spg} 791 \caption{\texttt{namdyn\_spg}} 792 \label{lst:namdyn_spg} 793 \end{listing} 781 794 %------------------------------------------------------------------------------------------------------------ 782 795 … … 884 897 %> > > > > > > > > > > > > > > > > > > > > > > > > > > > 885 898 \begin{figure}[!t] 886 \begin{center} 887 \includegraphics[width=\textwidth]{Fig_DYN_dynspg_ts} 888 \caption{ 889 \protect\label{fig:DYN_spg_ts} 890 Schematic of the split-explicit time stepping scheme for the external and internal modes. 891 Time increases to the right. In this particular exemple, 892 a boxcar averaging window over $nn\_baro$ barotropic time steps is used ($nn\_bt\_flt=1$) and $nn\_baro=5$. 893 Internal mode time steps (which are also the model time steps) are denoted by $t-\rdt$, $t$ and $t+\rdt$. 894 Variables with $k$ superscript refer to instantaneous barotropic variables, 895 $< >$ and $<< >>$ operator refer to time filtered variables using respectively primary (red vertical bars) and 896 secondary weights (blue vertical bars). 897 The former are used to obtain time filtered quantities at $t+\rdt$ while 898 the latter are used to obtain time averaged transports to advect tracers. 899 a) Forward time integration: \protect\np{ln\_bt\_fw}\forcode{=.true.}, 900 \protect\np{ln\_bt\_av}\forcode{=.true.}. 901 b) Centred time integration: \protect\np{ln\_bt\_fw}\forcode{=.false.}, 902 \protect\np{ln\_bt\_av}\forcode{=.true.}. 903 c) Forward time integration with no time filtering (POM-like scheme): 904 \protect\np{ln\_bt\_fw}\forcode{=.true.}, \protect\np{ln\_bt\_av}\forcode{=.false.}. 905 } 906 \end{center} 899 \centering 900 \includegraphics[width=\textwidth]{Fig_DYN_dynspg_ts} 901 \caption[Split-explicit time stepping scheme for the external and internal modes]{ 902 Schematic of the split-explicit time stepping scheme for the external and internal modes. 903 Time increases to the right. 904 In this particular exemple, 905 a boxcar averaging window over \np{nn\_baro} barotropic time steps is used 906 (\np{nn\_bt\_flt}\forcode{=1}) and \np{nn\_baro}\forcode{=5}. 907 Internal mode time steps (which are also the model time steps) are denoted by 908 $t-\rdt$, $t$ and $t+\rdt$. 909 Variables with $k$ superscript refer to instantaneous barotropic variables, 910 $< >$ and $<< >>$ operator refer to time filtered variables using respectively primary 911 (red vertical bars) and secondary weights (blue vertical bars). 912 The former are used to obtain time filtered quantities at $t+\rdt$ while 913 the latter are used to obtain time averaged transports to advect tracers. 914 a) Forward time integration: 915 \protect\np{ln\_bt\_fw}\forcode{=.true.}, \protect\np{ln\_bt\_av}\forcode{=.true.}. 916 b) Centred time integration: 917 \protect\np{ln\_bt\_fw}\forcode{=.false.}, \protect\np{ln\_bt\_av}\forcode{=.true.}. 918 c) Forward time integration with no time filtering (POM-like scheme): 919 \protect\np{ln\_bt\_fw}\forcode{=.true.}, \protect\np{ln\_bt\_av}\forcode{=.false.}.} 920 \label{fig:DYN_spg_ts} 907 921 \end{figure} 908 922 %> > > > > > > > > > > > > > > > > > > > > > > > > > > > … … 1114 1128 %------------------------------------------nam_dynldf---------------------------------------------------- 1115 1129 1116 \nlst{namdyn_ldf} 1130 \begin{listing} 1131 \nlst{namdyn_ldf} 1132 \caption{\texttt{namdyn\_ldf}} 1133 \label{lst:namdyn_ldf} 1134 \end{listing} 1117 1135 %------------------------------------------------------------------------------------------------------------- 1118 1136 … … 1245 1263 %----------------------------------------------namzdf------------------------------------------------------ 1246 1264 1247 \nlst{namzdf}1248 1265 %------------------------------------------------------------------------------------------------------------- 1249 1266 … … 1332 1349 by setting $\mathrm{ln\_wd\_dl} = \mathrm{.true.}$ and $\mathrm{ln\_wd\_il} = \mathrm{.false.}$. 1333 1350 1334 \nlst{namwad} 1351 \begin{listing} 1352 \nlst{namwad} 1353 \caption{\texttt{namwad}} 1354 \label{lst:namwad} 1355 \end{listing} 1335 1356 1336 1357 The following terminology is used. The depth of the topography (positive downwards) … … 1541 1562 neighbouring $(i+1,j)$ and $(i,j)$ tracer points. zcpx is calculated using two logicals 1542 1563 variables, $\mathrm{ll\_tmp1}$ and $\mathrm{ll\_tmp2}$ which are evaluated for each grid 1543 column. The three possible combinations are illustrated in figure\autoref{fig:DYN_WAD_dynhpg}.1564 column. The three possible combinations are illustrated in \autoref{fig:DYN_WAD_dynhpg}. 1544 1565 1545 1566 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>> 1546 \begin{figure}[!ht] \begin{center} 1547 \includegraphics[width=\textwidth]{Fig_WAD_dynhpg} 1548 \caption{ 1567 \begin{figure}[!ht] 1568 \centering 1569 \includegraphics[width=\textwidth]{Fig_WAD_dynhpg} 1570 \caption[Combinations controlling the limiting of the horizontal pressure gradient in 1571 wetting and drying regimes]{ 1572 Three possible combinations of the logical variables controlling the 1573 limiting of the horizontal pressure gradient in wetting and drying regimes} 1549 1574 \label{fig:DYN_WAD_dynhpg} 1550 Illustrations of the three possible combinations of the logical variables controlling the1551 limiting of the horizontal pressure gradient in wetting and drying regimes}1552 \end{center}1553 1575 \end{figure} 1554 1576 %>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>> … … 1625 1647 %----------------------------------------------namdom---------------------------------------------------- 1626 1648 1627 \nlst{namdom}1628 1649 %------------------------------------------------------------------------------------------------------------- 1629 1650
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