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% $Header: /u/gcmpack/manual/part3/getting_started.tex,v 1.22 2004/03/24 20:53:12 edhill Exp $ |
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% $Name: $ |
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|
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%\section{Getting started} |
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In this section, we describe how to use the model. In the first |
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section, we provide enough information to help you get started with |
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the model. We believe the best way to familiarize yourself with the |
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model is to run the case study examples provided with the base |
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version. Information on how to obtain, compile, and run the code is |
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found there as well as a brief description of the model structure |
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directory and the case study examples. The latter and the code |
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structure are described more fully in chapters |
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\ref{chap:discretization} and \ref{chap:sarch}, respectively. Here, in |
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this section, we provide information on how to customize the code when |
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you are ready to try implementing the configuration you have in mind. |
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\section{Where to find information} |
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\label{sect:whereToFindInfo} |
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A web site is maintained for release 2 (``Pelican'') of MITgcm: |
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\begin{rawhtml} <A href=http://mitgcm.org/pelican/ target="idontexist"> \end{rawhtml} |
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\begin{verbatim} |
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1.15 |
http://mitgcm.org/pelican |
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1.4 |
\end{verbatim} |
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\begin{rawhtml} </A> \end{rawhtml} |
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Here you will find an on-line version of this document, a |
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``browsable'' copy of the code and a searchable database of the model |
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and site, as well as links for downloading the model and |
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1.15 |
documentation, to data-sources, and other related sites. |
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1.4 |
|
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1.15 |
There is also a web-archived support mailing list for the model that |
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you can email at \texttt{MITgcm-support@mitgcm.org} or browse at: |
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\begin{rawhtml} <A href=http://mitgcm.org/mailman/listinfo/mitgcm-support/ target="idontexist"> \end{rawhtml} |
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\begin{verbatim} |
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http://mitgcm.org/mailman/listinfo/mitgcm-support/ |
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http://mitgcm.org/pipermail/mitgcm-support/ |
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\end{verbatim} |
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\begin{rawhtml} </A> \end{rawhtml} |
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Essentially all of the MITgcm web pages can be searched using a |
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popular web crawler such as Google or through our own search facility: |
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\begin{rawhtml} <A href=http://mitgcm.org/mailman/htdig/ target="idontexist"> \end{rawhtml} |
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\begin{verbatim} |
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http://mitgcm.org/htdig/ |
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\end{verbatim} |
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\begin{rawhtml} </A> \end{rawhtml} |
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%%% http://www.google.com/search?q=hydrostatic+site%3Amitgcm.org |
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\section{Obtaining the code} |
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\label{sect:obtainingCode} |
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|
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MITgcm can be downloaded from our system by following |
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the instructions below. As a courtesy we ask that you send e-mail to us at |
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\begin{rawhtml} <A href=mailto:MITgcm-support@mitgcm.org> \end{rawhtml} |
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MITgcm-support@mitgcm.org |
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\begin{rawhtml} </A> \end{rawhtml} |
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to enable us to keep track of who's using the model and in what application. |
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You can download the model two ways: |
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\begin{enumerate} |
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\item Using CVS software. CVS is a freely available source code management |
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tool. To use CVS you need to have the software installed. Many systems |
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come with CVS pre-installed, otherwise good places to look for |
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the software for a particular platform are |
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\begin{rawhtml} <A href=http://www.cvshome.org/ target="idontexist"> \end{rawhtml} |
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cvshome.org |
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\begin{rawhtml} </A> \end{rawhtml} |
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and |
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\begin{rawhtml} <A href=http://www.wincvs.org/ target="idontexist"> \end{rawhtml} |
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wincvs.org |
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\begin{rawhtml} </A> \end{rawhtml} |
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. |
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\item Using a tar file. This method is simple and does not |
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require any special software. However, this method does not |
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provide easy support for maintenance updates. |
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|
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\end{enumerate} |
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\subsubsection{Checkout from CVS} |
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\label{sect:cvs_checkout} |
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|
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If CVS is available on your system, we strongly encourage you to use it. CVS |
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provides an efficient and elegant way of organizing your code and keeping |
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track of your changes. If CVS is not available on your machine, you can also |
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download a tar file. |
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|
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Before you can use CVS, the following environment variable(s) should |
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be set within your shell. For a csh or tcsh shell, put the following |
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\begin{verbatim} |
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% setenv CVSROOT :pserver:cvsanon@mitgcm.org:/u/gcmpack |
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\end{verbatim} |
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in your .cshrc or .tcshrc file. For bash or sh shells, put: |
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\begin{verbatim} |
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% export CVSROOT=':pserver:cvsanon@mitgcm.org:/u/gcmpack' |
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\end{verbatim} |
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in your \texttt{.profile} or \texttt{.bashrc} file. |
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1.6 |
|
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|
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To get MITgcm through CVS, first register with the MITgcm CVS server |
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using command: |
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1.6 |
\begin{verbatim} |
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1.1 |
% cvs login ( CVS password: cvsanon ) |
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\end{verbatim} |
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You only need to do a ``cvs login'' once. |
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1.1 |
|
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To obtain the latest sources type: |
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\begin{verbatim} |
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% cvs co MITgcm |
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\end{verbatim} |
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or to get a specific release type: |
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\begin{verbatim} |
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% cvs co -P -r checkpoint52i_post MITgcm |
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\end{verbatim} |
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The MITgcm web site contains further directions concerning the source |
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code and CVS. It also contains a web interface to our CVS archive so |
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that one may easily view the state of files, revisions, and other |
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development milestones: |
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\begin{rawhtml} <A href=''http://mitgcm.org/download'' target="idontexist"> \end{rawhtml} |
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1.15 |
\begin{verbatim} |
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1.17 |
http://mitgcm.org/source_code.html |
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1.15 |
\end{verbatim} |
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\begin{rawhtml} </A> \end{rawhtml} |
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1.1 |
|
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1.19 |
As a convenience, the MITgcm CVS server contains aliases which are |
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named subsets of the codebase. These aliases can be especially |
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helpful when used over slow internet connections or on machines with |
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restricted storage space. Table \ref{tab:cvsModules} contains a list |
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of CVS aliases |
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\begin{table}[htb] |
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\centering |
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\begin{tabular}[htb]{|lp{3.25in}|}\hline |
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\textbf{Alias Name} & \textbf{Information (directories) Contained} \\\hline |
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\texttt{MITgcm\_code} & Only the source code -- none of the verification examples. \\ |
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\texttt{MITgcm\_verif\_basic} |
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& Source code plus a small set of the verification examples |
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(\texttt{global\_ocean.90x40x15}, \texttt{aim.5l\_cs}, \texttt{hs94.128x64x5}, |
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\texttt{front\_relax}, and \texttt{plume\_on\_slope}). \\ |
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\texttt{MITgcm\_verif\_atmos} & Source code plus all of the atmospheric examples. \\ |
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\texttt{MITgcm\_verif\_ocean} & Source code plus all of the oceanic examples. \\ |
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\texttt{MITgcm\_verif\_all} & Source code plus all of the |
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verification examples. \\\hline |
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\end{tabular} |
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\caption{MITgcm CVS Modules} |
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\label{tab:cvsModules} |
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\end{table} |
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1.15 |
|
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The checkout process creates a directory called \textit{MITgcm}. If |
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the directory \textit{MITgcm} exists this command updates your code |
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based on the repository. Each directory in the source tree contains a |
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directory \textit{CVS}. This information is required by CVS to keep |
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track of your file versions with respect to the repository. Don't edit |
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the files in \textit{CVS}! You can also use CVS to download code |
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updates. More extensive information on using CVS for maintaining |
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MITgcm code can be found |
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edhill |
1.17 |
\begin{rawhtml} <A href=''http://mitgcm.org/usingcvstoget.html'' target="idontexist"> \end{rawhtml} |
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cnh |
1.7 |
here |
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\begin{rawhtml} </A> \end{rawhtml} |
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. |
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edhill |
1.19 |
It is important to note that the CVS aliases in Table |
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\ref{tab:cvsModules} cannot be used in conjunction with the CVS |
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\texttt{-d DIRNAME} option. However, the \texttt{MITgcm} directories |
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they create can be changed to a different name following the check-out: |
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\begin{verbatim} |
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% cvs co MITgcm_verif_basic |
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% mv MITgcm MITgcm_verif_basic |
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\end{verbatim} |
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cnh |
1.7 |
|
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1.1 |
|
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edhill |
1.19 |
\subsubsection{Conventional download method} |
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1.4 |
\label{sect:conventionalDownload} |
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1.1 |
|
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1.4 |
If you do not have CVS on your system, you can download the model as a |
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edhill |
1.15 |
tar file from the web site at: |
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cnh |
1.7 |
\begin{rawhtml} <A href=http://mitgcm.org/download target="idontexist"> \end{rawhtml} |
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1.1 |
\begin{verbatim} |
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http://mitgcm.org/download/ |
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\end{verbatim} |
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1.7 |
\begin{rawhtml} </A> \end{rawhtml} |
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1.4 |
The tar file still contains CVS information which we urge you not to |
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delete; even if you do not use CVS yourself the information can help |
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1.15 |
us if you should need to send us your copy of the code. If a recent |
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tar file does not exist, then please contact the developers through |
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edhill |
1.17 |
the |
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\begin{rawhtml} <A href=''mailto:MITgcm-support@mitgcm.org"> \end{rawhtml} |
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MITgcm-support@mitgcm.org |
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\begin{rawhtml} </A> \end{rawhtml} |
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mailing list. |
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1.1 |
|
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1.19 |
\subsubsection{Upgrading from an earlier version} |
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1.12 |
|
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If you already have an earlier version of the code you can ``upgrade'' |
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your copy instead of downloading the entire repository again. First, |
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``cd'' (change directory) to the top of your working copy: |
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\begin{verbatim} |
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% cd MITgcm |
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\end{verbatim} |
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1.15 |
and then issue the cvs update command such as: |
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1.12 |
\begin{verbatim} |
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1.16 |
% cvs -q update -r checkpoint52i_post -d -P |
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1.12 |
\end{verbatim} |
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1.16 |
This will update the ``tag'' to ``checkpoint52i\_post'', add any new |
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1.12 |
directories (-d) and remove any empty directories (-P). The -q option |
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means be quiet which will reduce the number of messages you'll see in |
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the terminal. If you have modified the code prior to upgrading, CVS |
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will try to merge your changes with the upgrades. If there is a |
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conflict between your modifications and the upgrade, it will report |
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that file with a ``C'' in front, e.g.: |
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\begin{verbatim} |
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C model/src/ini_parms.F |
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\end{verbatim} |
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If the list of conflicts scrolled off the screen, you can re-issue the |
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cvs update command and it will report the conflicts. Conflicts are |
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edhill |
1.15 |
indicated in the code by the delimites ``$<<<<<<<$'', ``======='' and |
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``$>>>>>>>$''. For example, |
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1.17 |
{\small |
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1.12 |
\begin{verbatim} |
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<<<<<<< ini_parms.F |
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& bottomDragLinear,myOwnBottomDragCoefficient, |
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======= |
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& bottomDragLinear,bottomDragQuadratic, |
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>>>>>>> 1.18 |
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\end{verbatim} |
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edhill |
1.17 |
} |
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1.12 |
means that you added ``myOwnBottomDragCoefficient'' to a namelist at |
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the same time and place that we added ``bottomDragQuadratic''. You |
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need to resolve this conflict and in this case the line should be |
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changed to: |
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edhill |
1.17 |
{\small |
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1.12 |
\begin{verbatim} |
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& bottomDragLinear,bottomDragQuadratic,myOwnBottomDragCoefficient, |
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\end{verbatim} |
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edhill |
1.17 |
} |
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1.15 |
and the lines with the delimiters ($<<<<<<$,======,$>>>>>>$) be deleted. |
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adcroft |
1.12 |
Unless you are making modifications which exactly parallel |
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developments we make, these types of conflicts should be rare. |
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|
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\paragraph*{Upgrading to the current pre-release version} |
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|
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We don't make a ``release'' for every little patch and bug fix in |
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order to keep the frequency of upgrades to a minimum. However, if you |
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have run into a problem for which ``we have already fixed in the |
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latest code'' and we haven't made a ``tag'' or ``release'' since that |
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patch then you'll need to get the latest code: |
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\begin{verbatim} |
248 |
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% cvs -q update -A -d -P |
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\end{verbatim} |
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Unlike, the ``check-out'' and ``update'' procedures above, there is no |
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``tag'' or release name. The -A tells CVS to upgrade to the |
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very latest version. As a rule, we don't recommend this since you |
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might upgrade while we are in the processes of checking in the code so |
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that you may only have part of a patch. Using this method of updating |
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also means we can't tell what version of the code you are working |
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with. So please be sure you understand what you're doing. |
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|
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adcroft |
1.4 |
\section{Model and directory structure} |
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adcroft |
1.1 |
|
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1.12 |
The ``numerical'' model is contained within a execution environment |
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support wrapper. This wrapper is designed to provide a general |
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framework for grid-point models. MITgcmUV is a specific numerical |
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model that uses the framework. Under this structure the model is split |
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into execution environment support code and conventional numerical |
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model code. The execution environment support code is held under the |
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\textit{eesupp} directory. The grid point model code is held under the |
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\textit{model} directory. Code execution actually starts in the |
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\textit{eesupp} routines and not in the \textit{model} routines. For |
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edhill |
1.17 |
this reason the top-level \textit{MAIN.F} is in the |
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\textit{eesupp/src} directory. In general, end-users should not need |
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to worry about this level. The top-level routine for the numerical |
272 |
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part of the code is in \textit{model/src/THE\_MODEL\_MAIN.F}. Here is |
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a brief description of the directory structure of the model under the |
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root tree (a detailed description is given in section 3: Code |
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structure). |
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adcroft |
1.1 |
|
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\begin{itemize} |
278 |
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|
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1.17 |
\item \textit{bin}: this directory is initially empty. It is the |
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default directory in which to compile the code. |
281 |
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|
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adcroft |
1.1 |
\item \textit{diags}: contains the code relative to time-averaged |
283 |
edhill |
1.17 |
diagnostics. It is subdivided into two subdirectories \textit{inc} |
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and \textit{src} that contain include files (*.\textit{h} files) and |
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Fortran subroutines (*.\textit{F} files), respectively. |
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adcroft |
1.1 |
|
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\item \textit{doc}: contains brief documentation notes. |
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edhill |
1.17 |
|
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\item \textit{eesupp}: contains the execution environment source code. |
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Also subdivided into two subdirectories \textit{inc} and |
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\textit{src}. |
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|
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\item \textit{exe}: this directory is initially empty. It is the |
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default directory in which to execute the code. |
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|
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\item \textit{model}: this directory contains the main source code. |
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Also subdivided into two subdirectories \textit{inc} and |
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\textit{src}. |
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|
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\item \textit{pkg}: contains the source code for the packages. Each |
301 |
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package corresponds to a subdirectory. For example, \textit{gmredi} |
302 |
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contains the code related to the Gent-McWilliams/Redi scheme, |
303 |
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\textit{aim} the code relative to the atmospheric intermediate |
304 |
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physics. The packages are described in detail in section 3. |
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|
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\item \textit{tools}: this directory contains various useful tools. |
307 |
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For example, \textit{genmake2} is a script written in csh (C-shell) |
308 |
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that should be used to generate your makefile. The directory |
309 |
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\textit{adjoint} contains the makefile specific to the Tangent |
310 |
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linear and Adjoint Compiler (TAMC) that generates the adjoint code. |
311 |
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The latter is described in details in part V. |
312 |
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|
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adcroft |
1.1 |
\item \textit{utils}: this directory contains various utilities. The |
314 |
edhill |
1.17 |
subdirectory \textit{knudsen2} contains code and a makefile that |
315 |
|
|
compute coefficients of the polynomial approximation to the knudsen |
316 |
|
|
formula for an ocean nonlinear equation of state. The |
317 |
|
|
\textit{matlab} subdirectory contains matlab scripts for reading |
318 |
|
|
model output directly into matlab. \textit{scripts} contains C-shell |
319 |
|
|
post-processing scripts for joining processor-based and tiled-based |
320 |
|
|
model output. |
321 |
|
|
|
322 |
|
|
\item \textit{verification}: this directory contains the model |
323 |
|
|
examples. See section \ref{sect:modelExamples}. |
324 |
adcroft |
1.1 |
|
325 |
|
|
\end{itemize} |
326 |
|
|
|
327 |
adcroft |
1.4 |
\section{Example experiments} |
328 |
|
|
\label{sect:modelExamples} |
329 |
adcroft |
1.1 |
|
330 |
edhill |
1.15 |
%% a set of twenty-four pre-configured numerical experiments |
331 |
|
|
|
332 |
|
|
The MITgcm distribution comes with more than a dozen pre-configured |
333 |
|
|
numerical experiments. Some of these example experiments are tests of |
334 |
|
|
individual parts of the model code, but many are fully fledged |
335 |
|
|
numerical simulations. A few of the examples are used for tutorial |
336 |
|
|
documentation in sections \ref{sect:eg-baro} - \ref{sect:eg-global}. |
337 |
|
|
The other examples follow the same general structure as the tutorial |
338 |
|
|
examples. However, they only include brief instructions in a text file |
339 |
|
|
called {\it README}. The examples are located in subdirectories under |
340 |
|
|
the directory \textit{verification}. Each example is briefly described |
341 |
|
|
below. |
342 |
adcroft |
1.1 |
|
343 |
cnh |
1.8 |
\subsection{Full list of model examples} |
344 |
adcroft |
1.1 |
|
345 |
cnh |
1.8 |
\begin{enumerate} |
346 |
edhill |
1.17 |
|
347 |
adcroft |
1.1 |
\item \textit{exp0} - single layer, ocean double gyre (barotropic with |
348 |
edhill |
1.15 |
free-surface). This experiment is described in detail in section |
349 |
|
|
\ref{sect:eg-baro}. |
350 |
adcroft |
1.1 |
|
351 |
edhill |
1.15 |
\item \textit{exp1} - Four layer, ocean double gyre. This experiment |
352 |
|
|
is described in detail in section \ref{sect:eg-baroc}. |
353 |
|
|
|
354 |
adcroft |
1.1 |
\item \textit{exp2} - 4x4 degree global ocean simulation with steady |
355 |
edhill |
1.15 |
climatological forcing. This experiment is described in detail in |
356 |
|
|
section \ref{sect:eg-global}. |
357 |
|
|
|
358 |
|
|
\item \textit{exp4} - Flow over a Gaussian bump in open-water or |
359 |
|
|
channel with open boundaries. |
360 |
|
|
|
361 |
|
|
\item \textit{exp5} - Inhomogenously forced ocean convection in a |
362 |
|
|
doubly periodic box. |
363 |
adcroft |
1.1 |
|
364 |
cnh |
1.8 |
\item \textit{front\_relax} - Relaxation of an ocean thermal front (test for |
365 |
adcroft |
1.1 |
Gent/McWilliams scheme). 2D (Y-Z). |
366 |
|
|
|
367 |
edhill |
1.15 |
\item \textit{internal wave} - Ocean internal wave forced by open |
368 |
|
|
boundary conditions. |
369 |
|
|
|
370 |
cnh |
1.8 |
\item \textit{natl\_box} - Eastern subtropical North Atlantic with KPP |
371 |
edhill |
1.15 |
scheme; 1 month integration |
372 |
|
|
|
373 |
|
|
\item \textit{hs94.1x64x5} - Zonal averaged atmosphere using Held and |
374 |
|
|
Suarez '94 forcing. |
375 |
|
|
|
376 |
|
|
\item \textit{hs94.128x64x5} - 3D atmosphere dynamics using Held and |
377 |
|
|
Suarez '94 forcing. |
378 |
|
|
|
379 |
adcroft |
1.1 |
\item \textit{hs94.cs-32x32x5} - 3D atmosphere dynamics using Held and |
380 |
edhill |
1.15 |
Suarez '94 forcing on the cubed sphere. |
381 |
|
|
|
382 |
|
|
\item \textit{aim.5l\_zon-ave} - Intermediate Atmospheric physics. |
383 |
|
|
Global Zonal Mean configuration, 1x64x5 resolution. |
384 |
|
|
|
385 |
|
|
\item \textit{aim.5l\_XZ\_Equatorial\_Slice} - Intermediate |
386 |
|
|
Atmospheric physics, equatorial Slice configuration. 2D (X-Z). |
387 |
|
|
|
388 |
adcroft |
1.1 |
\item \textit{aim.5l\_Equatorial\_Channel} - Intermediate Atmospheric |
389 |
edhill |
1.15 |
physics. 3D Equatorial Channel configuration. |
390 |
|
|
|
391 |
cnh |
1.8 |
\item \textit{aim.5l\_LatLon} - Intermediate Atmospheric physics. |
392 |
edhill |
1.15 |
Global configuration, on latitude longitude grid with 128x64x5 grid |
393 |
|
|
points ($2.8^\circ{\rm degree}$ resolution). |
394 |
|
|
|
395 |
|
|
\item \textit{adjustment.128x64x1} Barotropic adjustment problem on |
396 |
|
|
latitude longitude grid with 128x64 grid points ($2.8^\circ{\rm |
397 |
|
|
degree}$ resolution). |
398 |
|
|
|
399 |
|
|
\item \textit{adjustment.cs-32x32x1} Barotropic adjustment problem on |
400 |
|
|
cube sphere grid with 32x32 points per face ( roughly $2.8^\circ{\rm |
401 |
|
|
degree}$ resolution). |
402 |
|
|
|
403 |
cnh |
1.8 |
\item \textit{advect\_cs} Two-dimensional passive advection test on |
404 |
edhill |
1.15 |
cube sphere grid. |
405 |
|
|
|
406 |
|
|
\item \textit{advect\_xy} Two-dimensional (horizontal plane) passive |
407 |
|
|
advection test on Cartesian grid. |
408 |
|
|
|
409 |
|
|
\item \textit{advect\_yz} Two-dimensional (vertical plane) passive |
410 |
|
|
advection test on Cartesian grid. |
411 |
|
|
|
412 |
|
|
\item \textit{carbon} Simple passive tracer experiment. Includes |
413 |
|
|
derivative calculation. Described in detail in section |
414 |
|
|
\ref{sect:eg-carbon-ad}. |
415 |
cnh |
1.8 |
|
416 |
|
|
\item \textit{flt\_example} Example of using float package. |
417 |
edhill |
1.15 |
|
418 |
|
|
\item \textit{global\_ocean.90x40x15} Global circulation with GM, flux |
419 |
|
|
boundary conditions and poles. |
420 |
cnh |
1.8 |
|
421 |
mlosch |
1.13 |
\item \textit{global\_ocean\_pressure} Global circulation in pressure |
422 |
|
|
coordinate (non-Boussinesq ocean model). Described in detail in |
423 |
|
|
section \ref{sect:eg-globalpressure}. |
424 |
edhill |
1.15 |
|
425 |
|
|
\item \textit{solid-body.cs-32x32x1} Solid body rotation test for cube |
426 |
|
|
sphere grid. |
427 |
cnh |
1.8 |
|
428 |
|
|
\end{enumerate} |
429 |
adcroft |
1.1 |
|
430 |
adcroft |
1.4 |
\subsection{Directory structure of model examples} |
431 |
adcroft |
1.1 |
|
432 |
|
|
Each example directory has the following subdirectories: |
433 |
|
|
|
434 |
|
|
\begin{itemize} |
435 |
|
|
\item \textit{code}: contains the code particular to the example. At a |
436 |
edhill |
1.16 |
minimum, this directory includes the following files: |
437 |
adcroft |
1.1 |
|
438 |
edhill |
1.16 |
\begin{itemize} |
439 |
|
|
\item \textit{code/CPP\_EEOPTIONS.h}: declares CPP keys relative to |
440 |
|
|
the ``execution environment'' part of the code. The default |
441 |
|
|
version is located in \textit{eesupp/inc}. |
442 |
|
|
|
443 |
|
|
\item \textit{code/CPP\_OPTIONS.h}: declares CPP keys relative to |
444 |
|
|
the ``numerical model'' part of the code. The default version is |
445 |
|
|
located in \textit{model/inc}. |
446 |
|
|
|
447 |
|
|
\item \textit{code/SIZE.h}: declares size of underlying |
448 |
|
|
computational grid. The default version is located in |
449 |
|
|
\textit{model/inc}. |
450 |
|
|
\end{itemize} |
451 |
|
|
|
452 |
|
|
In addition, other include files and subroutines might be present in |
453 |
|
|
\textit{code} depending on the particular experiment. See Section 2 |
454 |
|
|
for more details. |
455 |
edhill |
1.15 |
|
456 |
|
|
\item \textit{input}: contains the input data files required to run |
457 |
|
|
the example. At a minimum, the \textit{input} directory contains the |
458 |
|
|
following files: |
459 |
adcroft |
1.1 |
|
460 |
edhill |
1.16 |
\begin{itemize} |
461 |
|
|
\item \textit{input/data}: this file, written as a namelist, |
462 |
|
|
specifies the main parameters for the experiment. |
463 |
|
|
|
464 |
|
|
\item \textit{input/data.pkg}: contains parameters relative to the |
465 |
|
|
packages used in the experiment. |
466 |
|
|
|
467 |
|
|
\item \textit{input/eedata}: this file contains ``execution |
468 |
|
|
environment'' data. At present, this consists of a specification |
469 |
|
|
of the number of threads to use in $X$ and $Y$ under multithreaded |
470 |
|
|
execution. |
471 |
|
|
\end{itemize} |
472 |
edhill |
1.17 |
|
473 |
|
|
In addition, you will also find in this directory the forcing and |
474 |
|
|
topography files as well as the files describing the initial state |
475 |
|
|
of the experiment. This varies from experiment to experiment. See |
476 |
|
|
section 2 for more details. |
477 |
edhill |
1.16 |
|
478 |
|
|
\item \textit{results}: this directory contains the output file |
479 |
|
|
\textit{output.txt} produced by the simulation example. This file is |
480 |
|
|
useful for comparison with your own output when you run the |
481 |
|
|
experiment. |
482 |
adcroft |
1.1 |
\end{itemize} |
483 |
|
|
|
484 |
edhill |
1.17 |
Once you have chosen the example you want to run, you are ready to |
485 |
|
|
compile the code. |
486 |
adcroft |
1.1 |
|
487 |
adcroft |
1.4 |
\section{Building the code} |
488 |
|
|
\label{sect:buildingCode} |
489 |
|
|
|
490 |
|
|
To compile the code, we use the {\em make} program. This uses a file |
491 |
|
|
({\em Makefile}) that allows us to pre-process source files, specify |
492 |
|
|
compiler and optimization options and also figures out any file |
493 |
edhill |
1.16 |
dependencies. We supply a script ({\em genmake2}), described in |
494 |
|
|
section \ref{sect:genmake}, that automatically creates the {\em |
495 |
|
|
Makefile} for you. You then need to build the dependencies and |
496 |
|
|
compile the code. |
497 |
adcroft |
1.4 |
|
498 |
|
|
As an example, let's assume that you want to build and run experiment |
499 |
edhill |
1.16 |
\textit{verification/exp2}. The are multiple ways and places to |
500 |
|
|
actually do this but here let's build the code in |
501 |
adcroft |
1.4 |
\textit{verification/exp2/input}: |
502 |
|
|
\begin{verbatim} |
503 |
|
|
% cd verification/exp2/input |
504 |
|
|
\end{verbatim} |
505 |
|
|
First, build the {\em Makefile}: |
506 |
|
|
\begin{verbatim} |
507 |
edhill |
1.16 |
% ../../../tools/genmake2 -mods=../code |
508 |
adcroft |
1.4 |
\end{verbatim} |
509 |
|
|
The command line option tells {\em genmake} to override model source |
510 |
|
|
code with any files in the directory {\em ./code/}. |
511 |
|
|
|
512 |
edhill |
1.16 |
On many systems, the {\em genmake2} program will be able to |
513 |
|
|
automatically recognize the hardware, find compilers and other tools |
514 |
|
|
within the user's path (``echo \$PATH''), and then choose an |
515 |
|
|
appropriate set of options from the files contained in the {\em |
516 |
|
|
tools/build\_options} directory. Under some circumstances, a user |
517 |
|
|
may have to create a new ``optfile'' in order to specify the exact |
518 |
|
|
combination of compiler, compiler flags, libraries, and other options |
519 |
|
|
necessary to build a particular configuration of MITgcm. In such |
520 |
|
|
cases, it is generally helpful to read the existing ``optfiles'' and |
521 |
|
|
mimic their syntax. |
522 |
|
|
|
523 |
|
|
Through the MITgcm-support list, the MITgcm developers are willing to |
524 |
|
|
provide help writing or modifing ``optfiles''. And we encourage users |
525 |
|
|
to post new ``optfiles'' (particularly ones for new machines or |
526 |
edhill |
1.17 |
architectures) to the |
527 |
|
|
\begin{rawhtml} <A href=''mailto:MITgcm-support@mitgcm.org"> \end{rawhtml} |
528 |
|
|
MITgcm-support@mitgcm.org |
529 |
|
|
\begin{rawhtml} </A> \end{rawhtml} |
530 |
|
|
list. |
531 |
edhill |
1.16 |
|
532 |
|
|
To specify an optfile to {\em genmake2}, the syntax is: |
533 |
adcroft |
1.4 |
\begin{verbatim} |
534 |
edhill |
1.16 |
% ../../../tools/genmake2 -mods=../code -of /path/to/optfile |
535 |
adcroft |
1.4 |
\end{verbatim} |
536 |
|
|
|
537 |
edhill |
1.16 |
Once a {\em Makefile} has been generated, we create the dependencies: |
538 |
adcroft |
1.4 |
\begin{verbatim} |
539 |
|
|
% make depend |
540 |
|
|
\end{verbatim} |
541 |
edhill |
1.16 |
This modifies the {\em Makefile} by attaching a [long] list of files |
542 |
|
|
upon which other files depend. The purpose of this is to reduce |
543 |
|
|
re-compilation if and when you start to modify the code. The {\tt make |
544 |
|
|
depend} command also creates links from the model source to this |
545 |
|
|
directory. |
546 |
adcroft |
1.1 |
|
547 |
edhill |
1.16 |
Next compile the code: |
548 |
adcroft |
1.4 |
\begin{verbatim} |
549 |
|
|
% make |
550 |
|
|
\end{verbatim} |
551 |
|
|
The {\tt make} command creates an executable called \textit{mitgcmuv}. |
552 |
edhill |
1.16 |
Additional make ``targets'' are defined within the makefile to aid in |
553 |
|
|
the production of adjoint and other versions of MITgcm. |
554 |
adcroft |
1.4 |
|
555 |
|
|
Now you are ready to run the model. General instructions for doing so are |
556 |
|
|
given in section \ref{sect:runModel}. Here, we can run the model with: |
557 |
|
|
\begin{verbatim} |
558 |
|
|
./mitgcmuv > output.txt |
559 |
|
|
\end{verbatim} |
560 |
|
|
where we are re-directing the stream of text output to the file {\em |
561 |
|
|
output.txt}. |
562 |
|
|
|
563 |
|
|
|
564 |
|
|
\subsection{Building/compiling the code elsewhere} |
565 |
|
|
|
566 |
|
|
In the example above (section \ref{sect:buildingCode}) we built the |
567 |
|
|
executable in the {\em input} directory of the experiment for |
568 |
|
|
convenience. You can also configure and compile the code in other |
569 |
|
|
locations, for example on a scratch disk with out having to copy the |
570 |
|
|
entire source tree. The only requirement to do so is you have {\tt |
571 |
edhill |
1.16 |
genmake2} in your path or you know the absolute path to {\tt |
572 |
|
|
genmake2}. |
573 |
adcroft |
1.4 |
|
574 |
edhill |
1.16 |
The following sections outline some possible methods of organizing |
575 |
|
|
your source and data. |
576 |
adcroft |
1.4 |
|
577 |
|
|
\subsubsection{Building from the {\em ../code directory}} |
578 |
|
|
|
579 |
|
|
This is just as simple as building in the {\em input/} directory: |
580 |
|
|
\begin{verbatim} |
581 |
|
|
% cd verification/exp2/code |
582 |
edhill |
1.16 |
% ../../../tools/genmake2 |
583 |
adcroft |
1.4 |
% make depend |
584 |
|
|
% make |
585 |
|
|
\end{verbatim} |
586 |
|
|
However, to run the model the executable ({\em mitgcmuv}) and input |
587 |
|
|
files must be in the same place. If you only have one calculation to make: |
588 |
|
|
\begin{verbatim} |
589 |
|
|
% cd ../input |
590 |
|
|
% cp ../code/mitgcmuv ./ |
591 |
|
|
% ./mitgcmuv > output.txt |
592 |
|
|
\end{verbatim} |
593 |
cnh |
1.9 |
or if you will be making multiple runs with the same executable: |
594 |
adcroft |
1.4 |
\begin{verbatim} |
595 |
|
|
% cd ../ |
596 |
|
|
% cp -r input run1 |
597 |
|
|
% cp code/mitgcmuv run1 |
598 |
|
|
% cd run1 |
599 |
|
|
% ./mitgcmuv > output.txt |
600 |
|
|
\end{verbatim} |
601 |
|
|
|
602 |
|
|
\subsubsection{Building from a new directory} |
603 |
|
|
|
604 |
|
|
Since the {\em input} directory contains input files it is often more |
605 |
cnh |
1.9 |
useful to keep {\em input} pristine and build in a new directory |
606 |
adcroft |
1.4 |
within {\em verification/exp2/}: |
607 |
|
|
\begin{verbatim} |
608 |
|
|
% cd verification/exp2 |
609 |
|
|
% mkdir build |
610 |
|
|
% cd build |
611 |
edhill |
1.16 |
% ../../../tools/genmake2 -mods=../code |
612 |
adcroft |
1.4 |
% make depend |
613 |
|
|
% make |
614 |
|
|
\end{verbatim} |
615 |
|
|
This builds the code exactly as before but this time you need to copy |
616 |
|
|
either the executable or the input files or both in order to run the |
617 |
|
|
model. For example, |
618 |
|
|
\begin{verbatim} |
619 |
|
|
% cp ../input/* ./ |
620 |
|
|
% ./mitgcmuv > output.txt |
621 |
|
|
\end{verbatim} |
622 |
|
|
or if you tend to make multiple runs with the same executable then |
623 |
|
|
running in a new directory each time might be more appropriate: |
624 |
|
|
\begin{verbatim} |
625 |
|
|
% cd ../ |
626 |
|
|
% mkdir run1 |
627 |
|
|
% cp build/mitgcmuv run1/ |
628 |
|
|
% cp input/* run1/ |
629 |
|
|
% cd run1 |
630 |
|
|
% ./mitgcmuv > output.txt |
631 |
|
|
\end{verbatim} |
632 |
|
|
|
633 |
edhill |
1.16 |
\subsubsection{Building on a scratch disk} |
634 |
adcroft |
1.4 |
|
635 |
|
|
Model object files and output data can use up large amounts of disk |
636 |
|
|
space so it is often the case that you will be operating on a large |
637 |
|
|
scratch disk. Assuming the model source is in {\em ~/MITgcm} then the |
638 |
|
|
following commands will build the model in {\em /scratch/exp2-run1}: |
639 |
|
|
\begin{verbatim} |
640 |
|
|
% cd /scratch/exp2-run1 |
641 |
edhill |
1.16 |
% ~/MITgcm/tools/genmake2 -rootdir=~/MITgcm \ |
642 |
|
|
-mods=~/MITgcm/verification/exp2/code |
643 |
adcroft |
1.4 |
% make depend |
644 |
|
|
% make |
645 |
|
|
\end{verbatim} |
646 |
|
|
To run the model here, you'll need the input files: |
647 |
|
|
\begin{verbatim} |
648 |
|
|
% cp ~/MITgcm/verification/exp2/input/* ./ |
649 |
|
|
% ./mitgcmuv > output.txt |
650 |
|
|
\end{verbatim} |
651 |
|
|
|
652 |
|
|
As before, you could build in one directory and make multiple runs of |
653 |
|
|
the one experiment: |
654 |
|
|
\begin{verbatim} |
655 |
|
|
% cd /scratch/exp2 |
656 |
|
|
% mkdir build |
657 |
|
|
% cd build |
658 |
edhill |
1.16 |
% ~/MITgcm/tools/genmake2 -rootdir=~/MITgcm \ |
659 |
|
|
-mods=~/MITgcm/verification/exp2/code |
660 |
adcroft |
1.4 |
% make depend |
661 |
|
|
% make |
662 |
|
|
% cd ../ |
663 |
|
|
% cp -r ~/MITgcm/verification/exp2/input run2 |
664 |
|
|
% cd run2 |
665 |
|
|
% ./mitgcmuv > output.txt |
666 |
|
|
\end{verbatim} |
667 |
|
|
|
668 |
|
|
|
669 |
edhill |
1.16 |
\subsection{Using \textit{genmake2}} |
670 |
adcroft |
1.4 |
\label{sect:genmake} |
671 |
adcroft |
1.1 |
|
672 |
edhill |
1.16 |
To compile the code, first use the program \texttt{genmake2} (located |
673 |
|
|
in the \textit{tools} directory) to generate a Makefile. |
674 |
|
|
\texttt{genmake2} is a shell script written to work with all |
675 |
|
|
``sh''--compatible shells including bash v1, bash v2, and Bourne. |
676 |
|
|
Internally, \texttt{genmake2} determines the locations of needed |
677 |
|
|
files, the compiler, compiler options, libraries, and Unix tools. It |
678 |
|
|
relies upon a number of ``optfiles'' located in the {\em |
679 |
|
|
tools/build\_options} directory. |
680 |
|
|
|
681 |
|
|
The purpose of the optfiles is to provide all the compilation options |
682 |
|
|
for particular ``platforms'' (where ``platform'' roughly means the |
683 |
|
|
combination of the hardware and the compiler) and code configurations. |
684 |
|
|
Given the combinations of possible compilers and library dependencies |
685 |
|
|
({\it eg.} MPI and NetCDF) there may be numerous optfiles available |
686 |
|
|
for a single machine. The naming scheme for the majority of the |
687 |
|
|
optfiles shipped with the code is |
688 |
|
|
\begin{center} |
689 |
|
|
{\bf OS\_HARDWARE\_COMPILER } |
690 |
|
|
\end{center} |
691 |
|
|
where |
692 |
|
|
\begin{description} |
693 |
|
|
\item[OS] is the name of the operating system (generally the |
694 |
|
|
lower-case output of the {\tt 'uname'} command) |
695 |
|
|
\item[HARDWARE] is a string that describes the CPU type and |
696 |
|
|
corresponds to output from the {\tt 'uname -m'} command: |
697 |
|
|
\begin{description} |
698 |
|
|
\item[ia32] is for ``x86'' machines such as i386, i486, i586, i686, |
699 |
|
|
and athlon |
700 |
|
|
\item[ia64] is for Intel IA64 systems (eg. Itanium, Itanium2) |
701 |
|
|
\item[amd64] is AMD x86\_64 systems |
702 |
|
|
\item[ppc] is for Mac PowerPC systems |
703 |
|
|
\end{description} |
704 |
|
|
\item[COMPILER] is the compiler name (generally, the name of the |
705 |
|
|
FORTRAN executable) |
706 |
|
|
\end{description} |
707 |
|
|
|
708 |
|
|
In many cases, the default optfiles are sufficient and will result in |
709 |
|
|
usable Makefiles. However, for some machines or code configurations, |
710 |
|
|
new ``optfiles'' must be written. To create a new optfile, it is |
711 |
|
|
generally best to start with one of the defaults and modify it to suit |
712 |
|
|
your needs. Like \texttt{genmake2}, the optfiles are all written |
713 |
|
|
using a simple ``sh''--compatible syntax. While nearly all variables |
714 |
|
|
used within \texttt{genmake2} may be specified in the optfiles, the |
715 |
|
|
critical ones that should be defined are: |
716 |
|
|
|
717 |
|
|
\begin{description} |
718 |
|
|
\item[FC] the FORTRAN compiler (executable) to use |
719 |
|
|
\item[DEFINES] the command-line DEFINE options passed to the compiler |
720 |
|
|
\item[CPP] the C pre-processor to use |
721 |
|
|
\item[NOOPTFLAGS] options flags for special files that should not be |
722 |
|
|
optimized |
723 |
|
|
\end{description} |
724 |
|
|
|
725 |
|
|
For example, the optfile for a typical Red Hat Linux machine (``ia32'' |
726 |
|
|
architecture) using the GCC (g77) compiler is |
727 |
|
|
\begin{verbatim} |
728 |
|
|
FC=g77 |
729 |
|
|
DEFINES='-D_BYTESWAPIO -DWORDLENGTH=4' |
730 |
|
|
CPP='cpp -traditional -P' |
731 |
|
|
NOOPTFLAGS='-O0' |
732 |
|
|
# For IEEE, use the "-ffloat-store" option |
733 |
|
|
if test "x$IEEE" = x ; then |
734 |
|
|
FFLAGS='-Wimplicit -Wunused -Wuninitialized' |
735 |
|
|
FOPTIM='-O3 -malign-double -funroll-loops' |
736 |
|
|
else |
737 |
|
|
FFLAGS='-Wimplicit -Wunused -ffloat-store' |
738 |
|
|
FOPTIM='-O0 -malign-double' |
739 |
|
|
fi |
740 |
|
|
\end{verbatim} |
741 |
|
|
|
742 |
|
|
If you write an optfile for an unrepresented machine or compiler, you |
743 |
|
|
are strongly encouraged to submit the optfile to the MITgcm project |
744 |
|
|
for inclusion. Please send the file to the |
745 |
|
|
\begin{rawhtml} <A href="mail-to:MITgcm-support@mitgcm.org"> \end{rawhtml} |
746 |
|
|
\begin{center} |
747 |
|
|
MITgcm-support@mitgcm.org |
748 |
|
|
\end{center} |
749 |
|
|
\begin{rawhtml} </A> \end{rawhtml} |
750 |
|
|
mailing list. |
751 |
adcroft |
1.1 |
|
752 |
edhill |
1.16 |
In addition to the optfiles, \texttt{genmake2} supports a number of |
753 |
|
|
helpful command-line options. A complete list of these options can be |
754 |
|
|
obtained from: |
755 |
|
|
\begin{verbatim} |
756 |
|
|
% genmake2 -h |
757 |
|
|
\end{verbatim} |
758 |
|
|
|
759 |
|
|
The most important command-line options are: |
760 |
|
|
\begin{description} |
761 |
|
|
|
762 |
edhill |
1.17 |
\item[\texttt{--optfile=/PATH/FILENAME}] specifies the optfile that |
763 |
|
|
should be used for a particular build. |
764 |
edhill |
1.16 |
|
765 |
|
|
If no "optfile" is specified (either through the command line or the |
766 |
|
|
MITGCM\_OPTFILE environment variable), genmake2 will try to make a |
767 |
|
|
reasonable guess from the list provided in {\em |
768 |
|
|
tools/build\_options}. The method used for making this guess is |
769 |
|
|
to first determine the combination of operating system and hardware |
770 |
|
|
(eg. "linux\_ia32") and then find a working FORTRAN compiler within |
771 |
|
|
the user's path. When these three items have been identified, |
772 |
|
|
genmake2 will try to find an optfile that has a matching name. |
773 |
|
|
|
774 |
edhill |
1.22 |
\item[\texttt{--pdefault='PKG1 PKG2 PKG3 ...'}] specifies the default |
775 |
|
|
set of packages to be used. The normal order of precedence for |
776 |
|
|
packages is as follows: |
777 |
|
|
\begin{enumerate} |
778 |
|
|
\item If available, the command line (\texttt{--pdefault}) settings |
779 |
|
|
over-rule any others. |
780 |
|
|
|
781 |
|
|
\item Next, \texttt{genmake2} will look for a file named |
782 |
|
|
``\texttt{packages.conf}'' in the local directory or in any of the |
783 |
|
|
directories specified with the \texttt{--mods} option. |
784 |
|
|
|
785 |
|
|
\item Finally, if neither of the above are available, |
786 |
|
|
\texttt{genmake2} will use the \texttt{/pkg/pkg\_default} file. |
787 |
|
|
\end{enumerate} |
788 |
|
|
|
789 |
edhill |
1.17 |
\item[\texttt{--pdepend=/PATH/FILENAME}] specifies the dependency file |
790 |
|
|
used for packages. |
791 |
edhill |
1.16 |
|
792 |
|
|
If not specified, the default dependency file {\em pkg/pkg\_depend} |
793 |
|
|
is used. The syntax for this file is parsed on a line-by-line basis |
794 |
|
|
where each line containes either a comment ("\#") or a simple |
795 |
|
|
"PKGNAME1 (+|-)PKGNAME2" pairwise rule where the "+" or "-" symbol |
796 |
|
|
specifies a "must be used with" or a "must not be used with" |
797 |
|
|
relationship, respectively. If no rule is specified, then it is |
798 |
|
|
assumed that the two packages are compatible and will function |
799 |
|
|
either with or without each other. |
800 |
|
|
|
801 |
edhill |
1.17 |
\item[\texttt{--adof=/path/to/file}] specifies the "adjoint" or |
802 |
|
|
automatic differentiation options file to be used. The file is |
803 |
|
|
analogous to the ``optfile'' defined above but it specifies |
804 |
|
|
information for the AD build process. |
805 |
edhill |
1.16 |
|
806 |
|
|
The default file is located in {\em |
807 |
|
|
tools/adjoint\_options/adjoint\_default} and it defines the "TAF" |
808 |
|
|
and "TAMC" compilers. An alternate version is also available at |
809 |
|
|
{\em tools/adjoint\_options/adjoint\_staf} that selects the newer |
810 |
|
|
"STAF" compiler. As with any compilers, it is helpful to have their |
811 |
|
|
directories listed in your {\tt \$PATH} environment variable. |
812 |
|
|
|
813 |
edhill |
1.17 |
\item[\texttt{--mods='DIR1 DIR2 DIR3 ...'}] specifies a list of |
814 |
|
|
directories containing ``modifications''. These directories contain |
815 |
|
|
files with names that may (or may not) exist in the main MITgcm |
816 |
|
|
source tree but will be overridden by any identically-named sources |
817 |
|
|
within the ``MODS'' directories. |
818 |
edhill |
1.16 |
|
819 |
|
|
The order of precedence for this "name-hiding" is as follows: |
820 |
|
|
\begin{itemize} |
821 |
|
|
\item ``MODS'' directories (in the order given) |
822 |
|
|
\item Packages either explicitly specified or provided by default |
823 |
|
|
(in the order given) |
824 |
|
|
\item Packages included due to package dependencies (in the order |
825 |
|
|
that that package dependencies are parsed) |
826 |
|
|
\item The "standard dirs" (which may have been specified by the |
827 |
|
|
``-standarddirs'' option) |
828 |
|
|
\end{itemize} |
829 |
|
|
|
830 |
edhill |
1.23 |
\item[\texttt{--mpi}] This option enables certain MPI features (using |
831 |
|
|
CPP \texttt{\#define}s) within the code and is necessary for MPI |
832 |
|
|
builds (see Section \ref{sect:mpi-build}). |
833 |
|
|
|
834 |
edhill |
1.17 |
\item[\texttt{--make=/path/to/gmake}] Due to the poor handling of |
835 |
|
|
soft-links and other bugs common with the \texttt{make} versions |
836 |
|
|
provided by commercial Unix vendors, GNU \texttt{make} (sometimes |
837 |
|
|
called \texttt{gmake}) should be preferred. This option provides a |
838 |
|
|
means for specifying the make executable to be used. |
839 |
edhill |
1.21 |
|
840 |
|
|
\item[\texttt{--bash=/path/to/sh}] On some (usually older UNIX) |
841 |
|
|
machines, the ``bash'' shell is unavailable. To run on these |
842 |
|
|
systems, \texttt{genmake2} can be invoked using an ``sh'' (that is, |
843 |
|
|
a Bourne, POSIX, or compatible) shell. The syntax in these |
844 |
|
|
circumstances is: |
845 |
|
|
\begin{center} |
846 |
edhill |
1.23 |
\texttt{\% /bin/sh genmake2 -bash=/bin/sh [...options...]} |
847 |
edhill |
1.21 |
\end{center} |
848 |
|
|
where \texttt{/bin/sh} can be replaced with the full path and name |
849 |
|
|
of the desired shell. |
850 |
adcroft |
1.1 |
|
851 |
edhill |
1.16 |
\end{description} |
852 |
adcroft |
1.1 |
|
853 |
|
|
|
854 |
edhill |
1.23 |
\subsection{Building with MPI} |
855 |
|
|
\label{sect:mpi-build} |
856 |
|
|
|
857 |
|
|
Building MITgcm to use MPI libraries can be complicated due to the |
858 |
|
|
variety of different MPI implementations available, their dependencies |
859 |
|
|
or interactions with different compilers, and their often ad-hoc |
860 |
|
|
locations within file systems. For these reasons, its generally a |
861 |
|
|
good idea to start by finding and reading the documentation for your |
862 |
|
|
machine(s) and, if necessary, seeking help from your local systems |
863 |
|
|
administrator. |
864 |
|
|
|
865 |
|
|
The steps for building MITgcm with MPI support are: |
866 |
|
|
\begin{enumerate} |
867 |
|
|
|
868 |
|
|
\item Determine the locations of your MPI-enabled compiler and/or MPI |
869 |
|
|
libraries and put them into an options file as described in Section |
870 |
|
|
\ref{sect:genmake}. One can start with one of the examples in: |
871 |
|
|
\begin{rawhtml} <A |
872 |
|
|
href="http://mitgcm.org/cgi-bin/viewcvs.cgi/MITgcm/tools/build_options/"> |
873 |
|
|
\end{rawhtml} |
874 |
|
|
\begin{center} |
875 |
|
|
\texttt{MITgcm/tools/build\_options/} |
876 |
|
|
\end{center} |
877 |
|
|
\begin{rawhtml} </A> \end{rawhtml} |
878 |
|
|
such as \texttt{linux\_ia32\_g77+mpi\_cg01} or |
879 |
|
|
\texttt{linux\_ia64\_efc+mpi} and then edit it to suit the machine at |
880 |
|
|
hand. You may need help from your user guide or local systems |
881 |
|
|
administrator to determine the exact location of the MPI libraries. |
882 |
|
|
If libraries are not installed, MPI implementations and related |
883 |
|
|
tools are available including: |
884 |
|
|
\begin{itemize} |
885 |
|
|
\item \begin{rawhtml} <A |
886 |
|
|
href="http://www-unix.mcs.anl.gov/mpi/mpich/"> |
887 |
|
|
\end{rawhtml} |
888 |
|
|
MPICH |
889 |
|
|
\begin{rawhtml} </A> \end{rawhtml} |
890 |
|
|
|
891 |
|
|
\item \begin{rawhtml} <A |
892 |
|
|
href="http://www.lam-mpi.org/"> |
893 |
|
|
\end{rawhtml} |
894 |
|
|
LAM/MPI |
895 |
|
|
\begin{rawhtml} </A> \end{rawhtml} |
896 |
|
|
|
897 |
|
|
\item \begin{rawhtml} <A |
898 |
|
|
href="http://www.osc.edu/~pw/mpiexec/"> |
899 |
|
|
\end{rawhtml} |
900 |
|
|
MPIexec |
901 |
|
|
\begin{rawhtml} </A> \end{rawhtml} |
902 |
|
|
\end{itemize} |
903 |
|
|
|
904 |
|
|
\item Build the code with the \texttt{genmake2} \texttt{-mpi} option |
905 |
|
|
(see Section \ref{sect:genmake}) using commands such as: |
906 |
|
|
{\footnotesize \begin{verbatim} |
907 |
|
|
% ../../../tools/genmake2 -mods=../code -mpi -of=YOUR_OPTFILE |
908 |
|
|
% make depend |
909 |
|
|
% make |
910 |
|
|
\end{verbatim} } |
911 |
|
|
|
912 |
|
|
\item Run the code with the appropriate MPI ``run'' or ``exec'' |
913 |
|
|
program provided with your particular implementation of MPI. |
914 |
|
|
Typical MPI packages such as MPICH will use something like: |
915 |
|
|
\begin{verbatim} |
916 |
|
|
% mpirun -np 4 -machinefile mf ./mitgcmuv |
917 |
|
|
\end{verbatim} |
918 |
|
|
Sightly more complicated scripts may be needed for many machines |
919 |
|
|
since execution of the code may be controlled by both the MPI |
920 |
|
|
library and a job scheduling and queueing system such as PBS, |
921 |
|
|
LoadLeveller, Condor, or any of a number of similar tools. |
922 |
|
|
|
923 |
|
|
\end{enumerate} |
924 |
|
|
|
925 |
|
|
|
926 |
adcroft |
1.1 |
|
927 |
adcroft |
1.4 |
\section{Running the model} |
928 |
|
|
\label{sect:runModel} |
929 |
|
|
|
930 |
edhill |
1.23 |
If compilation finished succesfuully (section \ref{sect:buildingCode}) |
931 |
|
|
then an executable called \texttt{mitgcmuv} will now exist in the |
932 |
|
|
local directory. |
933 |
adcroft |
1.1 |
|
934 |
adcroft |
1.4 |
To run the model as a single process (ie. not in parallel) simply |
935 |
|
|
type: |
936 |
adcroft |
1.1 |
\begin{verbatim} |
937 |
adcroft |
1.4 |
% ./mitgcmuv |
938 |
adcroft |
1.1 |
\end{verbatim} |
939 |
adcroft |
1.4 |
The ``./'' is a safe-guard to make sure you use the local executable |
940 |
|
|
in case you have others that exist in your path (surely odd if you |
941 |
|
|
do!). The above command will spew out many lines of text output to |
942 |
|
|
your screen. This output contains details such as parameter values as |
943 |
|
|
well as diagnostics such as mean Kinetic energy, largest CFL number, |
944 |
|
|
etc. It is worth keeping this text output with the binary output so we |
945 |
|
|
normally re-direct the {\em stdout} stream as follows: |
946 |
adcroft |
1.1 |
\begin{verbatim} |
947 |
adcroft |
1.4 |
% ./mitgcmuv > output.txt |
948 |
adcroft |
1.1 |
\end{verbatim} |
949 |
|
|
|
950 |
edhill |
1.17 |
For the example experiments in {\em verification}, an example of the |
951 |
adcroft |
1.4 |
output is kept in {\em results/output.txt} for comparison. You can compare |
952 |
|
|
your {\em output.txt} with this one to check that the set-up works. |
953 |
adcroft |
1.1 |
|
954 |
|
|
|
955 |
|
|
|
956 |
adcroft |
1.4 |
\subsection{Output files} |
957 |
adcroft |
1.1 |
|
958 |
|
|
The model produces various output files. At a minimum, the instantaneous |
959 |
|
|
``state'' of the model is written out, which is made of the following files: |
960 |
|
|
|
961 |
|
|
\begin{itemize} |
962 |
|
|
\item \textit{U.00000nIter} - zonal component of velocity field (m/s and $> |
963 |
|
|
0 $ eastward). |
964 |
|
|
|
965 |
|
|
\item \textit{V.00000nIter} - meridional component of velocity field (m/s |
966 |
|
|
and $> 0$ northward). |
967 |
|
|
|
968 |
|
|
\item \textit{W.00000nIter} - vertical component of velocity field (ocean: |
969 |
|
|
m/s and $> 0$ upward, atmosphere: Pa/s and $> 0$ towards increasing pressure |
970 |
|
|
i.e. downward). |
971 |
|
|
|
972 |
|
|
\item \textit{T.00000nIter} - potential temperature (ocean: $^{0}$C, |
973 |
|
|
atmosphere: $^{0}$K). |
974 |
|
|
|
975 |
|
|
\item \textit{S.00000nIter} - ocean: salinity (psu), atmosphere: water vapor |
976 |
|
|
(g/kg). |
977 |
|
|
|
978 |
|
|
\item \textit{Eta.00000nIter} - ocean: surface elevation (m), atmosphere: |
979 |
|
|
surface pressure anomaly (Pa). |
980 |
|
|
\end{itemize} |
981 |
|
|
|
982 |
|
|
The chain \textit{00000nIter} consists of ten figures that specify the |
983 |
|
|
iteration number at which the output is written out. For example, \textit{% |
984 |
|
|
U.0000000300} is the zonal velocity at iteration 300. |
985 |
|
|
|
986 |
|
|
In addition, a ``pickup'' or ``checkpoint'' file called: |
987 |
|
|
|
988 |
|
|
\begin{itemize} |
989 |
|
|
\item \textit{pickup.00000nIter} |
990 |
|
|
\end{itemize} |
991 |
|
|
|
992 |
|
|
is written out. This file represents the state of the model in a condensed |
993 |
|
|
form and is used for restarting the integration. If the C-D scheme is used, |
994 |
|
|
there is an additional ``pickup'' file: |
995 |
|
|
|
996 |
|
|
\begin{itemize} |
997 |
|
|
\item \textit{pickup\_cd.00000nIter} |
998 |
|
|
\end{itemize} |
999 |
|
|
|
1000 |
|
|
containing the D-grid velocity data and that has to be written out as well |
1001 |
|
|
in order to restart the integration. Rolling checkpoint files are the same |
1002 |
|
|
as the pickup files but are named differently. Their name contain the chain |
1003 |
|
|
\textit{ckptA} or \textit{ckptB} instead of \textit{00000nIter}. They can be |
1004 |
|
|
used to restart the model but are overwritten every other time they are |
1005 |
|
|
output to save disk space during long integrations. |
1006 |
|
|
|
1007 |
adcroft |
1.4 |
\subsection{Looking at the output} |
1008 |
adcroft |
1.1 |
|
1009 |
|
|
All the model data are written according to a ``meta/data'' file format. |
1010 |
|
|
Each variable is associated with two files with suffix names \textit{.data} |
1011 |
|
|
and \textit{.meta}. The \textit{.data} file contains the data written in |
1012 |
|
|
binary form (big\_endian by default). The \textit{.meta} file is a |
1013 |
|
|
``header'' file that contains information about the size and the structure |
1014 |
|
|
of the \textit{.data} file. This way of organizing the output is |
1015 |
|
|
particularly useful when running multi-processors calculations. The base |
1016 |
|
|
version of the model includes a few matlab utilities to read output files |
1017 |
|
|
written in this format. The matlab scripts are located in the directory |
1018 |
|
|
\textit{utils/matlab} under the root tree. The script \textit{rdmds.m} reads |
1019 |
|
|
the data. Look at the comments inside the script to see how to use it. |
1020 |
|
|
|
1021 |
adcroft |
1.4 |
Some examples of reading and visualizing some output in {\em Matlab}: |
1022 |
|
|
\begin{verbatim} |
1023 |
|
|
% matlab |
1024 |
|
|
>> H=rdmds('Depth'); |
1025 |
|
|
>> contourf(H');colorbar; |
1026 |
|
|
>> title('Depth of fluid as used by model'); |
1027 |
|
|
|
1028 |
|
|
>> eta=rdmds('Eta',10); |
1029 |
|
|
>> imagesc(eta');axis ij;colorbar; |
1030 |
|
|
>> title('Surface height at iter=10'); |
1031 |
|
|
|
1032 |
|
|
>> eta=rdmds('Eta',[0:10:100]); |
1033 |
|
|
>> for n=1:11; imagesc(eta(:,:,n)');axis ij;colorbar;pause(.5);end |
1034 |
|
|
\end{verbatim} |
1035 |
adcroft |
1.1 |
|
1036 |
|
|
\section{Doing it yourself: customizing the code} |
1037 |
|
|
|
1038 |
|
|
When you are ready to run the model in the configuration you want, the |
1039 |
edhill |
1.17 |
easiest thing is to use and adapt the setup of the case studies |
1040 |
|
|
experiment (described previously) that is the closest to your |
1041 |
|
|
configuration. Then, the amount of setup will be minimized. In this |
1042 |
|
|
section, we focus on the setup relative to the ``numerical model'' |
1043 |
|
|
part of the code (the setup relative to the ``execution environment'' |
1044 |
|
|
part is covered in the parallel implementation section) and on the |
1045 |
|
|
variables and parameters that you are likely to change. |
1046 |
adcroft |
1.1 |
|
1047 |
adcroft |
1.5 |
\subsection{Configuration and setup} |
1048 |
adcroft |
1.4 |
|
1049 |
edhill |
1.17 |
The CPP keys relative to the ``numerical model'' part of the code are |
1050 |
|
|
all defined and set in the file \textit{CPP\_OPTIONS.h }in the |
1051 |
|
|
directory \textit{ model/inc }or in one of the \textit{code |
1052 |
|
|
}directories of the case study experiments under |
1053 |
|
|
\textit{verification.} The model parameters are defined and declared |
1054 |
|
|
in the file \textit{model/inc/PARAMS.h }and their default values are |
1055 |
|
|
set in the routine \textit{model/src/set\_defaults.F. }The default |
1056 |
|
|
values can be modified in the namelist file \textit{data }which needs |
1057 |
|
|
to be located in the directory where you will run the model. The |
1058 |
|
|
parameters are initialized in the routine |
1059 |
|
|
\textit{model/src/ini\_parms.F}. Look at this routine to see in what |
1060 |
|
|
part of the namelist the parameters are located. |
1061 |
|
|
|
1062 |
|
|
In what follows the parameters are grouped into categories related to |
1063 |
|
|
the computational domain, the equations solved in the model, and the |
1064 |
|
|
simulation controls. |
1065 |
adcroft |
1.1 |
|
1066 |
adcroft |
1.4 |
\subsection{Computational domain, geometry and time-discretization} |
1067 |
adcroft |
1.1 |
|
1068 |
edhill |
1.17 |
\begin{description} |
1069 |
|
|
\item[dimensions] \ |
1070 |
|
|
|
1071 |
edhill |
1.18 |
The number of points in the x, y, and r directions are represented |
1072 |
|
|
by the variables \textbf{sNx}, \textbf{sNy} and \textbf{Nr} |
1073 |
|
|
respectively which are declared and set in the file |
1074 |
|
|
\textit{model/inc/SIZE.h}. (Again, this assumes a mono-processor |
1075 |
|
|
calculation. For multiprocessor calculations see the section on |
1076 |
|
|
parallel implementation.) |
1077 |
edhill |
1.17 |
|
1078 |
|
|
\item[grid] \ |
1079 |
|
|
|
1080 |
|
|
Three different grids are available: cartesian, spherical polar, and |
1081 |
edhill |
1.18 |
curvilinear (which includes the cubed sphere). The grid is set |
1082 |
|
|
through the logical variables \textbf{usingCartesianGrid}, |
1083 |
|
|
\textbf{usingSphericalPolarGrid}, and \textbf{usingCurvilinearGrid}. |
1084 |
|
|
In the case of spherical and curvilinear grids, the southern |
1085 |
|
|
boundary is defined through the variable \textbf{phiMin} which |
1086 |
|
|
corresponds to the latitude of the southern most cell face (in |
1087 |
|
|
degrees). The resolution along the x and y directions is controlled |
1088 |
|
|
by the 1D arrays \textbf{delx} and \textbf{dely} (in meters in the |
1089 |
|
|
case of a cartesian grid, in degrees otherwise). The vertical grid |
1090 |
|
|
spacing is set through the 1D array \textbf{delz} for the ocean (in |
1091 |
|
|
meters) or \textbf{delp} for the atmosphere (in Pa). The variable |
1092 |
|
|
\textbf{Ro\_SeaLevel} represents the standard position of Sea-Level |
1093 |
|
|
in ``R'' coordinate. This is typically set to 0m for the ocean |
1094 |
|
|
(default value) and 10$^{5}$Pa for the atmosphere. For the |
1095 |
|
|
atmosphere, also set the logical variable \textbf{groundAtK1} to |
1096 |
|
|
\texttt{'.TRUE.'} which puts the first level (k=1) at the lower |
1097 |
edhill |
1.17 |
boundary (ground). |
1098 |
|
|
|
1099 |
|
|
For the cartesian grid case, the Coriolis parameter $f$ is set |
1100 |
edhill |
1.18 |
through the variables \textbf{f0} and \textbf{beta} which correspond |
1101 |
|
|
to the reference Coriolis parameter (in s$^{-1}$) and |
1102 |
|
|
$\frac{\partial f}{ \partial y}$(in m$^{-1}$s$^{-1}$) respectively. |
1103 |
|
|
If \textbf{beta } is set to a nonzero value, \textbf{f0} is the |
1104 |
|
|
value of $f$ at the southern edge of the domain. |
1105 |
edhill |
1.17 |
|
1106 |
|
|
\item[topography - full and partial cells] \ |
1107 |
|
|
|
1108 |
|
|
The domain bathymetry is read from a file that contains a 2D (x,y) |
1109 |
|
|
map of depths (in m) for the ocean or pressures (in Pa) for the |
1110 |
|
|
atmosphere. The file name is represented by the variable |
1111 |
edhill |
1.18 |
\textbf{bathyFile}. The file is assumed to contain binary numbers |
1112 |
|
|
giving the depth (pressure) of the model at each grid cell, ordered |
1113 |
|
|
with the x coordinate varying fastest. The points are ordered from |
1114 |
|
|
low coordinate to high coordinate for both axes. The model code |
1115 |
|
|
applies without modification to enclosed, periodic, and double |
1116 |
|
|
periodic domains. Periodicity is assumed by default and is |
1117 |
edhill |
1.17 |
suppressed by setting the depths to 0m for the cells at the limits |
1118 |
|
|
of the computational domain (note: not sure this is the case for the |
1119 |
|
|
atmosphere). The precision with which to read the binary data is |
1120 |
edhill |
1.18 |
controlled by the integer variable \textbf{readBinaryPrec} which can |
1121 |
edhill |
1.17 |
take the value \texttt{32} (single precision) or \texttt{64} (double |
1122 |
edhill |
1.18 |
precision). See the matlab program \textit{gendata.m} in the |
1123 |
|
|
\textit{input} directories under \textit{verification} to see how |
1124 |
edhill |
1.17 |
the bathymetry files are generated for the case study experiments. |
1125 |
|
|
|
1126 |
edhill |
1.18 |
To use the partial cell capability, the variable \textbf{hFacMin} |
1127 |
|
|
needs to be set to a value between 0 and 1 (it is set to 1 by |
1128 |
|
|
default) corresponding to the minimum fractional size of the cell. |
1129 |
|
|
For example if the bottom cell is 500m thick and \textbf{hFacMin} is |
1130 |
|
|
set to 0.1, the actual thickness of the cell (i.e. used in the code) |
1131 |
|
|
can cover a range of discrete values 50m apart from 50m to 500m |
1132 |
|
|
depending on the value of the bottom depth (in \textbf{bathyFile}) |
1133 |
|
|
at this point. |
1134 |
edhill |
1.17 |
|
1135 |
|
|
Note that the bottom depths (or pressures) need not coincide with |
1136 |
edhill |
1.18 |
the models levels as deduced from \textbf{delz} or \textbf{delp}. |
1137 |
|
|
The model will interpolate the numbers in \textbf{bathyFile} so that |
1138 |
|
|
they match the levels obtained from \textbf{delz} or \textbf{delp} |
1139 |
|
|
and \textbf{hFacMin}. |
1140 |
edhill |
1.17 |
|
1141 |
|
|
(Note: the atmospheric case is a bit more complicated than what is |
1142 |
|
|
written here I think. To come soon...) |
1143 |
|
|
|
1144 |
|
|
\item[time-discretization] \ |
1145 |
|
|
|
1146 |
|
|
The time steps are set through the real variables \textbf{deltaTMom} |
1147 |
|
|
and \textbf{deltaTtracer} (in s) which represent the time step for |
1148 |
|
|
the momentum and tracer equations, respectively. For synchronous |
1149 |
|
|
integrations, simply set the two variables to the same value (or you |
1150 |
|
|
can prescribe one time step only through the variable |
1151 |
|
|
\textbf{deltaT}). The Adams-Bashforth stabilizing parameter is set |
1152 |
|
|
through the variable \textbf{abEps} (dimensionless). The stagger |
1153 |
|
|
baroclinic time stepping can be activated by setting the logical |
1154 |
edhill |
1.18 |
variable \textbf{staggerTimeStep} to \texttt{'.TRUE.'}. |
1155 |
adcroft |
1.1 |
|
1156 |
edhill |
1.17 |
\end{description} |
1157 |
adcroft |
1.1 |
|
1158 |
|
|
|
1159 |
adcroft |
1.4 |
\subsection{Equation of state} |
1160 |
adcroft |
1.1 |
|
1161 |
mlosch |
1.13 |
First, because the model equations are written in terms of |
1162 |
|
|
perturbations, a reference thermodynamic state needs to be specified. |
1163 |
|
|
This is done through the 1D arrays \textbf{tRef} and \textbf{sRef}. |
1164 |
|
|
\textbf{tRef} specifies the reference potential temperature profile |
1165 |
|
|
(in $^{o}$C for the ocean and $^{o}$K for the atmosphere) starting |
1166 |
|
|
from the level k=1. Similarly, \textbf{sRef} specifies the reference |
1167 |
|
|
salinity profile (in ppt) for the ocean or the reference specific |
1168 |
|
|
humidity profile (in g/kg) for the atmosphere. |
1169 |
|
|
|
1170 |
|
|
The form of the equation of state is controlled by the character |
1171 |
|
|
variables \textbf{buoyancyRelation} and \textbf{eosType}. |
1172 |
edhill |
1.18 |
\textbf{buoyancyRelation} is set to \texttt{'OCEANIC'} by default and |
1173 |
|
|
needs to be set to \texttt{'ATMOSPHERIC'} for atmosphere simulations. |
1174 |
|
|
In this case, \textbf{eosType} must be set to \texttt{'IDEALGAS'}. |
1175 |
mlosch |
1.13 |
For the ocean, two forms of the equation of state are available: |
1176 |
edhill |
1.18 |
linear (set \textbf{eosType} to \texttt{'LINEAR'}) and a polynomial |
1177 |
|
|
approximation to the full nonlinear equation ( set \textbf{eosType} to |
1178 |
|
|
\texttt{'POLYNOMIAL'}). In the linear case, you need to specify the |
1179 |
|
|
thermal and haline expansion coefficients represented by the variables |
1180 |
|
|
\textbf{tAlpha} (in K$^{-1}$) and \textbf{sBeta} (in ppt$^{-1}$). For |
1181 |
|
|
the nonlinear case, you need to generate a file of polynomial |
1182 |
|
|
coefficients called \textit{POLY3.COEFFS}. To do this, use the program |
1183 |
mlosch |
1.13 |
\textit{utils/knudsen2/knudsen2.f} under the model tree (a Makefile is |
1184 |
|
|
available in the same directory and you will need to edit the number |
1185 |
|
|
and the values of the vertical levels in \textit{knudsen2.f} so that |
1186 |
|
|
they match those of your configuration). |
1187 |
|
|
|
1188 |
|
|
There there are also higher polynomials for the equation of state: |
1189 |
|
|
\begin{description} |
1190 |
edhill |
1.18 |
\item[\texttt{'UNESCO'}:] The UNESCO equation of state formula of |
1191 |
mlosch |
1.13 |
Fofonoff and Millard \cite{fofonoff83}. This equation of state |
1192 |
edhill |
1.18 |
assumes in-situ temperature, which is not a model variable; {\em its |
1193 |
|
|
use is therefore discouraged, and it is only listed for |
1194 |
|
|
completeness}. |
1195 |
|
|
\item[\texttt{'JMD95Z'}:] A modified UNESCO formula by Jackett and |
1196 |
mlosch |
1.13 |
McDougall \cite{jackett95}, which uses the model variable potential |
1197 |
edhill |
1.18 |
temperature as input. The \texttt{'Z'} indicates that this equation |
1198 |
mlosch |
1.13 |
of state uses a horizontally and temporally constant pressure |
1199 |
|
|
$p_{0}=-g\rho_{0}z$. |
1200 |
edhill |
1.18 |
\item[\texttt{'JMD95P'}:] A modified UNESCO formula by Jackett and |
1201 |
mlosch |
1.13 |
McDougall \cite{jackett95}, which uses the model variable potential |
1202 |
edhill |
1.18 |
temperature as input. The \texttt{'P'} indicates that this equation |
1203 |
mlosch |
1.13 |
of state uses the actual hydrostatic pressure of the last time |
1204 |
|
|
step. Lagging the pressure in this way requires an additional pickup |
1205 |
|
|
file for restarts. |
1206 |
edhill |
1.18 |
\item[\texttt{'MDJWF'}:] The new, more accurate and less expensive |
1207 |
mlosch |
1.13 |
equation of state by McDougall et~al. \cite{mcdougall03}. It also |
1208 |
|
|
requires lagging the pressure and therefore an additional pickup |
1209 |
|
|
file for restarts. |
1210 |
|
|
\end{description} |
1211 |
|
|
For none of these options an reference profile of temperature or |
1212 |
|
|
salinity is required. |
1213 |
adcroft |
1.1 |
|
1214 |
adcroft |
1.4 |
\subsection{Momentum equations} |
1215 |
adcroft |
1.1 |
|
1216 |
edhill |
1.18 |
In this section, we only focus for now on the parameters that you are |
1217 |
|
|
likely to change, i.e. the ones relative to forcing and dissipation |
1218 |
|
|
for example. The details relevant to the vector-invariant form of the |
1219 |
|
|
equations and the various advection schemes are not covered for the |
1220 |
|
|
moment. We assume that you use the standard form of the momentum |
1221 |
|
|
equations (i.e. the flux-form) with the default advection scheme. |
1222 |
|
|
Also, there are a few logical variables that allow you to turn on/off |
1223 |
|
|
various terms in the momentum equation. These variables are called |
1224 |
|
|
\textbf{momViscosity, momAdvection, momForcing, useCoriolis, |
1225 |
|
|
momPressureForcing, momStepping} and \textbf{metricTerms }and are |
1226 |
|
|
assumed to be set to \texttt{'.TRUE.'} here. Look at the file |
1227 |
|
|
\textit{model/inc/PARAMS.h }for a precise definition of these |
1228 |
|
|
variables. |
1229 |
adcroft |
1.1 |
|
1230 |
edhill |
1.17 |
\begin{description} |
1231 |
|
|
\item[initialization] \ |
1232 |
|
|
|
1233 |
|
|
The velocity components are initialized to 0 unless the simulation |
1234 |
|
|
is starting from a pickup file (see section on simulation control |
1235 |
|
|
parameters). |
1236 |
|
|
|
1237 |
|
|
\item[forcing] \ |
1238 |
|
|
|
1239 |
|
|
This section only applies to the ocean. You need to generate |
1240 |
edhill |
1.18 |
wind-stress data into two files \textbf{zonalWindFile} and |
1241 |
|
|
\textbf{meridWindFile} corresponding to the zonal and meridional |
1242 |
edhill |
1.17 |
components of the wind stress, respectively (if you want the stress |
1243 |
|
|
to be along the direction of only one of the model horizontal axes, |
1244 |
|
|
you only need to generate one file). The format of the files is |
1245 |
|
|
similar to the bathymetry file. The zonal (meridional) stress data |
1246 |
|
|
are assumed to be in Pa and located at U-points (V-points). As for |
1247 |
|
|
the bathymetry, the precision with which to read the binary data is |
1248 |
edhill |
1.18 |
controlled by the variable \textbf{readBinaryPrec}. See the matlab |
1249 |
|
|
program \textit{gendata.m} in the \textit{input} directories under |
1250 |
|
|
\textit{verification} to see how simple analytical wind forcing data |
1251 |
|
|
are generated for the case study experiments. |
1252 |
edhill |
1.17 |
|
1253 |
|
|
There is also the possibility of prescribing time-dependent periodic |
1254 |
|
|
forcing. To do this, concatenate the successive time records into a |
1255 |
edhill |
1.18 |
single file (for each stress component) ordered in a (x,y,t) fashion |
1256 |
|
|
and set the following variables: \textbf{periodicExternalForcing }to |
1257 |
|
|
\texttt{'.TRUE.'}, \textbf{externForcingPeriod }to the period (in s) |
1258 |
|
|
of which the forcing varies (typically 1 month), and |
1259 |
|
|
\textbf{externForcingCycle} to the repeat time (in s) of the forcing |
1260 |
|
|
(typically 1 year -- note: \textbf{ externForcingCycle} must be a |
1261 |
|
|
multiple of \textbf{externForcingPeriod}). With these variables set |
1262 |
|
|
up, the model will interpolate the forcing linearly at each |
1263 |
|
|
iteration. |
1264 |
edhill |
1.17 |
|
1265 |
|
|
\item[dissipation] \ |
1266 |
|
|
|
1267 |
|
|
The lateral eddy viscosity coefficient is specified through the |
1268 |
edhill |
1.18 |
variable \textbf{viscAh} (in m$^{2}$s$^{-1}$). The vertical eddy |
1269 |
|
|
viscosity coefficient is specified through the variable |
1270 |
|
|
\textbf{viscAz} (in m$^{2}$s$^{-1}$) for the ocean and |
1271 |
|
|
\textbf{viscAp} (in Pa$^{2}$s$^{-1}$) for the atmosphere. The |
1272 |
|
|
vertical diffusive fluxes can be computed implicitly by setting the |
1273 |
|
|
logical variable \textbf{implicitViscosity }to \texttt{'.TRUE.'}. |
1274 |
|
|
In addition, biharmonic mixing can be added as well through the |
1275 |
|
|
variable \textbf{viscA4} (in m$^{4}$s$^{-1}$). On a spherical polar |
1276 |
|
|
grid, you might also need to set the variable \textbf{cosPower} |
1277 |
|
|
which is set to 0 by default and which represents the power of |
1278 |
|
|
cosine of latitude to multiply viscosity. Slip or no-slip conditions |
1279 |
|
|
at lateral and bottom boundaries are specified through the logical |
1280 |
|
|
variables \textbf{no\_slip\_sides} and \textbf{no\_slip\_bottom}. If |
1281 |
|
|
set to \texttt{'.FALSE.'}, free-slip boundary conditions are |
1282 |
|
|
applied. If no-slip boundary conditions are applied at the bottom, a |
1283 |
|
|
bottom drag can be applied as well. Two forms are available: linear |
1284 |
|
|
(set the variable \textbf{bottomDragLinear} in s$ ^{-1}$) and |
1285 |
|
|
quadratic (set the variable \textbf{bottomDragQuadratic} in |
1286 |
|
|
m$^{-1}$). |
1287 |
edhill |
1.17 |
|
1288 |
|
|
The Fourier and Shapiro filters are described elsewhere. |
1289 |
|
|
|
1290 |
|
|
\item[C-D scheme] \ |
1291 |
|
|
|
1292 |
|
|
If you run at a sufficiently coarse resolution, you will need the |
1293 |
|
|
C-D scheme for the computation of the Coriolis terms. The |
1294 |
|
|
variable\textbf{\ tauCD}, which represents the C-D scheme coupling |
1295 |
|
|
timescale (in s) needs to be set. |
1296 |
|
|
|
1297 |
|
|
\item[calculation of pressure/geopotential] \ |
1298 |
|
|
|
1299 |
|
|
First, to run a non-hydrostatic ocean simulation, set the logical |
1300 |
edhill |
1.18 |
variable \textbf{nonHydrostatic} to \texttt{'.TRUE.'}. The pressure |
1301 |
edhill |
1.17 |
field is then inverted through a 3D elliptic equation. (Note: this |
1302 |
|
|
capability is not available for the atmosphere yet.) By default, a |
1303 |
|
|
hydrostatic simulation is assumed and a 2D elliptic equation is used |
1304 |
|
|
to invert the pressure field. The parameters controlling the |
1305 |
|
|
behaviour of the elliptic solvers are the variables |
1306 |
edhill |
1.18 |
\textbf{cg2dMaxIters} and \textbf{cg2dTargetResidual } for |
1307 |
|
|
the 2D case and \textbf{cg3dMaxIters} and |
1308 |
|
|
\textbf{cg3dTargetResidual} for the 3D case. You probably won't need to |
1309 |
edhill |
1.17 |
alter the default values (are we sure of this?). |
1310 |
|
|
|
1311 |
|
|
For the calculation of the surface pressure (for the ocean) or |
1312 |
|
|
surface geopotential (for the atmosphere) you need to set the |
1313 |
edhill |
1.18 |
logical variables \textbf{rigidLid} and \textbf{implicitFreeSurface} |
1314 |
|
|
(set one to \texttt{'.TRUE.'} and the other to \texttt{'.FALSE.'} |
1315 |
|
|
depending on how you want to deal with the ocean upper or atmosphere |
1316 |
|
|
lower boundary). |
1317 |
adcroft |
1.1 |
|
1318 |
edhill |
1.17 |
\end{description} |
1319 |
adcroft |
1.1 |
|
1320 |
adcroft |
1.4 |
\subsection{Tracer equations} |
1321 |
adcroft |
1.1 |
|
1322 |
edhill |
1.18 |
This section covers the tracer equations i.e. the potential |
1323 |
|
|
temperature equation and the salinity (for the ocean) or specific |
1324 |
|
|
humidity (for the atmosphere) equation. As for the momentum equations, |
1325 |
|
|
we only describe for now the parameters that you are likely to change. |
1326 |
|
|
The logical variables \textbf{tempDiffusion} \textbf{tempAdvection} |
1327 |
|
|
\textbf{tempForcing}, and \textbf{tempStepping} allow you to turn |
1328 |
|
|
on/off terms in the temperature equation (same thing for salinity or |
1329 |
|
|
specific humidity with variables \textbf{saltDiffusion}, |
1330 |
|
|
\textbf{saltAdvection} etc.). These variables are all assumed here to |
1331 |
|
|
be set to \texttt{'.TRUE.'}. Look at file \textit{model/inc/PARAMS.h} |
1332 |
|
|
for a precise definition. |
1333 |
adcroft |
1.1 |
|
1334 |
edhill |
1.17 |
\begin{description} |
1335 |
|
|
\item[initialization] \ |
1336 |
|
|
|
1337 |
|
|
The initial tracer data can be contained in the binary files |
1338 |
edhill |
1.18 |
\textbf{hydrogThetaFile} and \textbf{hydrogSaltFile}. These files |
1339 |
|
|
should contain 3D data ordered in an (x,y,r) fashion with k=1 as the |
1340 |
|
|
first vertical level. If no file names are provided, the tracers |
1341 |
|
|
are then initialized with the values of \textbf{tRef} and |
1342 |
|
|
\textbf{sRef} mentioned above (in the equation of state section). In |
1343 |
edhill |
1.17 |
this case, the initial tracer data are uniform in x and y for each |
1344 |
|
|
depth level. |
1345 |
|
|
|
1346 |
|
|
\item[forcing] \ |
1347 |
|
|
|
1348 |
|
|
This part is more relevant for the ocean, the procedure for the |
1349 |
|
|
atmosphere not being completely stabilized at the moment. |
1350 |
|
|
|
1351 |
|
|
A combination of fluxes data and relaxation terms can be used for |
1352 |
edhill |
1.18 |
driving the tracer equations. For potential temperature, heat flux |
1353 |
edhill |
1.17 |
data (in W/m$ ^{2}$) can be stored in the 2D binary file |
1354 |
edhill |
1.18 |
\textbf{surfQfile}. Alternatively or in addition, the forcing can |
1355 |
|
|
be specified through a relaxation term. The SST data to which the |
1356 |
|
|
model surface temperatures are restored to are supposed to be stored |
1357 |
|
|
in the 2D binary file \textbf{thetaClimFile}. The corresponding |
1358 |
|
|
relaxation time scale coefficient is set through the variable |
1359 |
|
|
\textbf{tauThetaClimRelax} (in s). The same procedure applies for |
1360 |
|
|
salinity with the variable names \textbf{EmPmRfile}, |
1361 |
|
|
\textbf{saltClimFile}, and \textbf{tauSaltClimRelax} for freshwater |
1362 |
|
|
flux (in m/s) and surface salinity (in ppt) data files and |
1363 |
|
|
relaxation time scale coefficient (in s), respectively. Also for |
1364 |
|
|
salinity, if the CPP key \textbf{USE\_NATURAL\_BCS} is turned on, |
1365 |
|
|
natural boundary conditions are applied i.e. when computing the |
1366 |
|
|
surface salinity tendency, the freshwater flux is multiplied by the |
1367 |
|
|
model surface salinity instead of a constant salinity value. |
1368 |
edhill |
1.17 |
|
1369 |
|
|
As for the other input files, the precision with which to read the |
1370 |
|
|
data is controlled by the variable \textbf{readBinaryPrec}. |
1371 |
|
|
Time-dependent, periodic forcing can be applied as well following |
1372 |
|
|
the same procedure used for the wind forcing data (see above). |
1373 |
|
|
|
1374 |
|
|
\item[dissipation] \ |
1375 |
|
|
|
1376 |
|
|
Lateral eddy diffusivities for temperature and salinity/specific |
1377 |
edhill |
1.18 |
humidity are specified through the variables \textbf{diffKhT} and |
1378 |
|
|
\textbf{diffKhS} (in m$^{2}$/s). Vertical eddy diffusivities are |
1379 |
|
|
specified through the variables \textbf{diffKzT} and |
1380 |
|
|
\textbf{diffKzS} (in m$^{2}$/s) for the ocean and \textbf{diffKpT |
1381 |
|
|
}and \textbf{diffKpS} (in Pa$^{2}$/s) for the atmosphere. The |
1382 |
|
|
vertical diffusive fluxes can be computed implicitly by setting the |
1383 |
|
|
logical variable \textbf{implicitDiffusion} to \texttt{'.TRUE.'}. |
1384 |
|
|
In addition, biharmonic diffusivities can be specified as well |
1385 |
|
|
through the coefficients \textbf{diffK4T} and \textbf{diffK4S} (in |
1386 |
edhill |
1.17 |
m$^{4}$/s). Note that the cosine power scaling (specified through |
1387 |
edhill |
1.18 |
\textbf{cosPower}---see the momentum equations section) is applied to |
1388 |
|
|
the tracer diffusivities (Laplacian and biharmonic) as well. The |
1389 |
edhill |
1.17 |
Gent and McWilliams parameterization for oceanic tracers is |
1390 |
|
|
described in the package section. Finally, note that tracers can be |
1391 |
|
|
also subject to Fourier and Shapiro filtering (see the corresponding |
1392 |
|
|
section on these filters). |
1393 |
|
|
|
1394 |
|
|
\item[ocean convection] \ |
1395 |
|
|
|
1396 |
|
|
Two options are available to parameterize ocean convection: one is |
1397 |
|
|
to use the convective adjustment scheme. In this case, you need to |
1398 |
|
|
set the variable \textbf{cadjFreq}, which represents the frequency |
1399 |
|
|
(in s) with which the adjustment algorithm is called, to a non-zero |
1400 |
|
|
value (if set to a negative value by the user, the model will set it |
1401 |
|
|
to the tracer time step). The other option is to parameterize |
1402 |
|
|
convection with implicit vertical diffusion. To do this, set the |
1403 |
edhill |
1.18 |
logical variable \textbf{implicitDiffusion} to \texttt{'.TRUE.'} |
1404 |
|
|
and the real variable \textbf{ivdc\_kappa} to a value (in m$^{2}$/s) |
1405 |
edhill |
1.17 |
you wish the tracer vertical diffusivities to have when mixing |
1406 |
|
|
tracers vertically due to static instabilities. Note that |
1407 |
edhill |
1.18 |
\textbf{cadjFreq} and \textbf{ivdc\_kappa}can not both have non-zero |
1408 |
|
|
value. |
1409 |
adcroft |
1.1 |
|
1410 |
edhill |
1.17 |
\end{description} |
1411 |
adcroft |
1.1 |
|
1412 |
adcroft |
1.4 |
\subsection{Simulation controls} |
1413 |
adcroft |
1.1 |
|
1414 |
edhill |
1.18 |
The model ''clock'' is defined by the variable \textbf{deltaTClock} |
1415 |
|
|
(in s) which determines the IO frequencies and is used in tagging |
1416 |
|
|
output. Typically, you will set it to the tracer time step for |
1417 |
|
|
accelerated runs (otherwise it is simply set to the default time step |
1418 |
|
|
\textbf{deltaT}). Frequency of checkpointing and dumping of the model |
1419 |
|
|
state are referenced to this clock (see below). |
1420 |
adcroft |
1.1 |
|
1421 |
edhill |
1.17 |
\begin{description} |
1422 |
|
|
\item[run duration] \ |
1423 |
|
|
|
1424 |
|
|
The beginning of a simulation is set by specifying a start time (in |
1425 |
edhill |
1.18 |
s) through the real variable \textbf{startTime} or by specifying an |
1426 |
edhill |
1.17 |
initial iteration number through the integer variable |
1427 |
|
|
\textbf{nIter0}. If these variables are set to nonzero values, the |
1428 |
edhill |
1.18 |
model will look for a ''pickup'' file \textit{pickup.0000nIter0} to |
1429 |
|
|
restart the integration. The end of a simulation is set through the |
1430 |
|
|
real variable \textbf{endTime} (in s). Alternatively, you can |
1431 |
|
|
specify instead the number of time steps to execute through the |
1432 |
|
|
integer variable \textbf{nTimeSteps}. |
1433 |
edhill |
1.17 |
|
1434 |
|
|
\item[frequency of output] \ |
1435 |
|
|
|
1436 |
|
|
Real variables defining frequencies (in s) with which output files |
1437 |
edhill |
1.18 |
are written on disk need to be set up. \textbf{dumpFreq} controls |
1438 |
edhill |
1.17 |
the frequency with which the instantaneous state of the model is |
1439 |
edhill |
1.18 |
saved. \textbf{chkPtFreq} and \textbf{pchkPtFreq} control the output |
1440 |
|
|
frequency of rolling and permanent checkpoint files, respectively. |
1441 |
|
|
See section 1.5.1 Output files for the definition of model state and |
1442 |
|
|
checkpoint files. In addition, time-averaged fields can be written |
1443 |
|
|
out by setting the variable \textbf{taveFreq} (in s). The precision |
1444 |
|
|
with which to write the binary data is controlled by the integer |
1445 |
|
|
variable w\textbf{riteBinaryPrec} (set it to \texttt{32} or |
1446 |
|
|
\texttt{64}). |
1447 |
adcroft |
1.1 |
|
1448 |
edhill |
1.17 |
\end{description} |
1449 |
adcroft |
1.1 |
|
1450 |
mlosch |
1.13 |
|
1451 |
|
|
%%% Local Variables: |
1452 |
|
|
%%% mode: latex |
1453 |
|
|
%%% TeX-master: t |
1454 |
|
|
%%% End: |