s_examples/held_suarez_cs/inp_data.shap.templ


%\subsubsection{File {\it input/data.pkg}}
%\label{www:tutorials}

This file, reproduced completely below, specifies the parameters
that the model uses for the Shapiro filter package (\cite{Shapiro_70},
section \ref{sect:shapiro-filter}).
The parameters that are significant for this configuration are:

\begin{itemize}

\item Line PUT_LINE_NB:Shap_funct=,
\begin{verbatim} 
 Shap_funct=2,
\end{verbatim} 
This line selects the shapiro filter function
to use, here S2 in this experiment
(see section \ref{sect:shapiro-filter}).

\item Lines PUT_LINE_NB:nShapT= and PUT_LINE_NB:nShapUV=,
\begin{verbatim}
 nShapT=4,
 nShapUV=4,
\end{verbatim}
Those lines select the order of the shapiro filter
for active tracer ($\theta$ and $q$) and momentum respectively. 
This sets the integer parameter $n$ to 4, in the equations of 
section \ref{sect:shapiro-filter}, which implies a 8th order
filter.

\item Lines PUT_LINE_NB:nShapTrPhys= and PUT_LINE_NB:nShapUVPhys=,
\begin{verbatim}
 nShapTrPhys=0,
 nShapUVPhys=0,
\end{verbatim}
Those lines select the order of the physical space filter 
(filter function S2g, in section \ref{sect:shapiro-filter})
that applies to for $\theta$ and $q$ and for $u$ and $v$ respectively.
The difference $ nShapT - nShapTrPhys $ and $ nShapUV - nShapUVPhys $
correspond to the order of the computational filter
(filter function S2c, in section \ref{sect:shapiro-filter}).

\item Lines PUT_LINE_NB:Shap_Trtau= and PUT_LINE_NB:Shap_uvtau=,
\begin{verbatim}
 Shap_Trtau=5400.,
 Shap_uvtau=1800.,
\end{verbatim}
Thoses lines set the time scale of the filter (in seconds), 
for $\theta$ and $q$ and for $u$ and $v$ respectively,
to 5400 s (90 min) and 1800 s (30 min) respectively.
Note that a shorter time scale means a stronger filter, and
that the time scale cannot be smaller than the time-step $\Delta t$
of the model.

\end{itemize}

The entire file {\it input/data.shap} is reproduced here below:
1	jmc	1.1
2			%\subsubsection{File {\it input/data.pkg}}
3			%\label{www:tutorials}
4
5			This file, reproduced completely below, specifies the parameters
6			that the model uses for the Shapiro filter package (\cite{Shapiro_70},
7			section \ref{sect:shapiro-filter}).
8			The parameters that are significant for this configuration are:
9
10			\begin{itemize}
11
12			\item Line PUT_LINE_NB:Shap_funct=,
13			\begin{verbatim}
14			Shap_funct=2,
15			\end{verbatim}
16			This line selects the shapiro filter function
17			to use, here S2 in this experiment
18			(see section \ref{sect:shapiro-filter}).
19
20			\item Lines PUT_LINE_NB:nShapT= and PUT_LINE_NB:nShapUV=,
21			\begin{verbatim}
22			nShapT=4,
23			nShapUV=4,
24			\end{verbatim}
25			Those lines select the order of the shapiro filter
26			for active tracer ($\theta$ and $q$) and momentum respectively.
27			This sets the integer parameter $n$ to 4, in the equations of
28			section \ref{sect:shapiro-filter}, which implies a 8th order
29			filter.
30
31			\item Lines PUT_LINE_NB:nShapTrPhys= and PUT_LINE_NB:nShapUVPhys=,
32			\begin{verbatim}
33			nShapTrPhys=0,
34			nShapUVPhys=0,
35			\end{verbatim}
36			Those lines select the order of the physical space filter
37			(filter function S2g, in section \ref{sect:shapiro-filter})
38			that applies to for $\theta$ and $q$ and for $u$ and $v$ respectively.
39			The difference $ nShapT - nShapTrPhys $ and $ nShapUV - nShapUVPhys $
40			correspond to the order of the computational filter
41			(filter function S2c, in section \ref{sect:shapiro-filter}).
42
43			\item Lines PUT_LINE_NB:Shap_Trtau= and PUT_LINE_NB:Shap_uvtau=,
44			\begin{verbatim}
45			Shap_Trtau=5400.,
46			Shap_uvtau=1800.,
47			\end{verbatim}
48			Thoses lines set the time scale of the filter (in seconds),
49			for $\theta$ and $q$ and for $u$ and $v$ respectively,
50			to 5400 s (90 min) and 1800 s (30 min) respectively.
51			Note that a shorter time scale means a stronger filter, and
52			that the time scale cannot be smaller than the time-step $\Delta t$
53			of the model.
54
55			\end{itemize}
56
57			The entire file {\it input/data.shap} is reproduced here below: