Changeset 9392 for branches/2017/dev_merge_2017/DOC/tex_sub/chap_time_domain.tex

Timestamp:

2018-03-09T16:57:00+01:00 (6 years ago)

Author:

nicolasmartin

Message:

Global replacement of patterns \np{id}=value by \forcode{id = value} for integer and booleans

File:

• branches/2017/dev_merge_2017/DOC/tex_sub/chap_time_domain.tex (modified) (4 diffs)

branches/2017/dev_merge_2017/DOC/tex_sub/chap_time_domain.tex

@@ -91 +91 @@
 \end{equation} 
 where the subscript $F$ denotes filtered values and $\gamma$ is the Asselin 
-coefficient. $\gamma$ is initialized as \np{rn\_atfp} (namelist parameter). 
-Its default value is \np{rn\_atfp}=$10^{-3}$ (see \S~\ref{STP_mLF}), 
+coefficient. $\gamma$ is initialized as \np{rn_atfp} (namelist parameter). 
+Its default value is \np{rn_atfp}=$10^{-3}$ (see \S~\ref{STP_mLF}), 
 causing only a weak dissipation of high frequency motions (\citep{Farge1987}). 
 The addition of a time filter degrades the accuracy of the 
@@ -141 +141 @@
 constraint on the time step. Two solutions are available in \NEMO to overcome 
 the stability constraint: $(a)$ a forward time differencing scheme using a 
-time splitting technique (\np{ln\_zdfexp} = true) or $(b)$ a backward (or implicit) 
-time differencing scheme (\np{ln\_zdfexp} = false). In $(a)$, the master 
+time splitting technique (\np{ln_zdfexp} = true) or $(b)$ a backward (or implicit) 
+time differencing scheme (\np{ln_zdfexp} = false). In $(a)$, the master 
 time step $\Delta $t is cut into $N$ fractional time steps so that the 
 stability criterion is reduced by a factor of $N$. The computation is performed as 
@@ -156 +156 @@
 \end{equation}
 with DF a vertical diffusion term. The number of fractional time steps, $N$, is given 
-by setting \np{nn\_zdfexp}, (namelist parameter). The scheme $(b)$ is unconditionally 
+by setting \np{nn_zdfexp}, (namelist parameter). The scheme $(b)$ is unconditionally 
 stable but diffusive. It can be written as follows:
 \begin{equation} \label{Eq_STP_imp}
@@ -309 +309 @@
 gradient (see \S\ref{DYN_hpg_imp}), an extra three-dimensional field has to be 
 added to the restart file to ensure an exact restartability. This is done optionally 
-via the  \np{nn\_dynhpg\_rst} namelist parameter, so that the size of the
+via the  \np{nn_dynhpg_rst} namelist parameter, so that the size of the
 restart file can be reduced when restartability is not a key issue (operational 
 oceanography or in ensemble simulations for seasonal forecasting).