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- The {\bf P}ortable {\bf U}niversity {\bf M}odel of the
- {\bf A}tmosphere {\bf (PUMA)} is based on the multi-level spectral
- model {\bf SGCM} ({\bf S}imple {\bf G}lobal {\bf C}irculation
- {\bf M}odel) described by \citep{hossim75} and \citep{jamesgray86}.
- Originally developed as a numerical prediction model,
- it was changed to perform as a circulation model. For example,
- \citep{jamesgray86} studied the influence of surface friction
- on the circulation of a baroclinic atmosphere, \citep{jamesjames92}
- and \citep{JamFraeJam94} investigated ultra-low-frequency
- variability, and \citep{molejames90} analyzed the baroclinic
- adjustment in the context of a zonally varying flow. \citep{frisius98}
- simulated an idealized storm track by embedding
- a dipole structure in a zonally symmetric forcing field and \citep{lunkeit98}
- investigated the sensitivity of GCM scenarios by using
- an adaption technique applicable to SGCMs.
- Storm track dynamics and low frequency variability
- was investigated by \citep{fraedrich2005}. For further citations search the
- bibliography at the end of this document and the list of publications at
- {\url{http://www.mi.uni-hamburg.de/puma}}.
-
- PUMA was created with following aims in mind: training of junior
- scientists, compatibility with the {\bf ECHAM}
- ({\bf E}uropean {\bf C}entre - {\bf HAM}burg) model and as a tool for
- further scientific investigations.
-
- \section{Training of junior scientists and students}
- PUMA contains only the main processes necessary to simulate
- the atmosphere. The source code is short and clearly arranged.
- A student can learn to work with PUMA within a few weeks, whereas a
- full size GCM requires a team of specialists for maintenance,
- experiment design and diagnostics.
-
- \section{Compatibility with other models}
- PUMA is designed to be compatible with other
- circulation models like Planet Simulator and ECHAM.
- The same triangular truncation is employed,
- and analogous transformation techniques like the Legendre- and
- Fast-Fourier transformation are used.
- The postprocessor {\bf Pumaburner} differs from ECHAM's
- {\bf Afterburner} only in respect to the format of the model's
- raw data which overcomes some problems of the ECHAM data format.
- PUMA uses a more compact though more precise
- format compared to the {\bf GRIB} ({\bf GRI}dded {\bf B}inary),
- which is used for ECHAM output.
- The Pumaburner supports the output formats SERVICE and
- NetCDF. All diagnostics and graphics software that are used with the
- ECHAM/Afterburner data can be used with PUMA/Pumaburner
- in exactly the same way.
- \pagebreak
-
- \begin{figure}
- \centering
- \begin{minipage}{0.75\linewidth}
- \includegraphics[height=15cm]{Pics/Processes_ECHAM}
- %\centering \epsfig{figure=Tr_z.Eng.eps, width=\linewidth}
- \end{minipage}
- \setlength{\unitlength}{1cm}
- \vspace{-2cm}
- \begin{minipage}{.5\linewidth}
- \begin{picture}(6,8)
- \thicklines
- \newsavebox{\ovalbox}
- \savebox{\ovalbox}(0,0){
- \thicklines
- \put(0,-0.5){\oval(2.0,0.7)}}
- \newsavebox{\frbox}
- \savebox{\frbox}(0,0){
- \thicklines
- \put(0,-0.5){\framebox(2.0,0.7)}}
- \put(4,4.2){\usebox{\ovalbox}}
- \put(3.35,3.95){\scriptsize \shortstack[c]{Adiabatic \\ processes}}
- \put(4,3.75){\vector(3,-2){1.5}}
- \put(5.5,2.75){\vector(-3,2){1.5}}
- \put(4,3.75){\vector(-3,-2){1.5}}
- \put(2.5,2.75){\vector(3,2){1.5}}
- \put(1.5,2.4){\usebox{\frbox}\makebox(2.05,0){\scriptsize Winds}}
- \put(4.5,2.4){\usebox{\frbox}\makebox(2.1,0){\scriptsize Temperature}}
- \put(2.5,2.05){\vector(0,-1){1.05}}
- \put(2.5,1.05){\vector(0,1){1.}}
- \put(5.5,2.05){\vector(0,-1){1.05}}
- \put(5.5,1.05){\vector(0,1){1.}}
- \put(2.5,0.7){\usebox{\ovalbox}}
- \put(2.5,0.6){\makebox(0,0){\scriptsize Friction}}
- \put(5.5,0.7){\usebox{\ovalbox}}
- \put(4.95,0.4){\scriptsize \shortstack[c]{Diabatic \\ heating}}
- \end{picture}
- \end{minipage}
- \vspace{1cm}
- \caption{Processes in ECHAM (a) and PUMA (b)}
- \label{ProcessesFig}
- \end{figure}
- \section{Scientific applications}
- The PUMA code is the dynamical core of a GCM forced by Newtonian
- cooling and Rayleigh friction, such as that proposed by Held \&
- Suarez (1994) to evaluate the dynamical cores of GCMs. It forms
- the basis for various applications:
- \begin{itemize}
- \item The code can be utilized
- to build and test new numerical algorithms (like semi-Langrangian
- techniques).
- \item Idealized experiments can be performed to analyze nonlinear
- processes arising from internal atmospheric systems (life cycles,
- etc.).
- \item Data assimilation techniques can be incorporated to
- interpret results from GCM simulations or observations.
- \end{itemize}
- Figure \ref{ProcessesFig} (a) demonstrates the complexity of the
- interactions in a full size climate model, which leads to similar
- complex response patterns from small parameter changes. The same
- diagram for PUMA Figure \ref{ProcessesFig} (b) shows the simple
- and direct paths which allow the easy identification of the effects
- from changes to this model.
- \section{Requirements}
- PUMA is open source, everyone may download and use it.
- Though it's easy to use,
- the design of experiments and the interpretation of the results
- require a thorough knowledge of atmospheric science.
- PUMA is available as FORTRAN-90 source code. So all that is needed
- to use PUMA on any computer is a FORTRAN-90 compiler.
- The GUI additionally requires a C-compiler with the graphical
- library X11, which is standard on any UNIX/Linux system
- as well as on newer MACs.
- Windows user may try a X11-emulator like Cygwin.
- The program was developed and tested with several operating systems
- including LINUX, MAC-OS, and Solaris. The main development was done
- using Linux and MAC-OS and the FORTRAN compiler gfortran and sunf90.
- The postprocessor Pumaburner requires a C++ compiler.
- There are several compilers available for the Linux operating system.
- MoSt, PUMA, and Planet Simulator were successfully tested with:
- \begin{itemize}
- \item SunStudio12 (development environment including
- FORTRAN-90, C, C++, and Debugger) for Solaris and Linux.
- SunStudio12 can be downloaded for free from {\url{http://www.sun.com}}.
- \item Gnu FORTRAN (gfortran).
- This free and open access FORTRAN-90 compiler is part of most
- Linux distributions.
- It's also available from
- {\url{http://directory.fsf.org/devel/compilers/gfortran.html}}.
- \end{itemize}
- \section{History}
-
- The University of Hamburg PUMA model originates from
- the Hoskins \& Simmons SGCM ({\bf S}imple {\bf G}eneral {\bf C}irculation {\bf M}odel)
- version (\citep{hossim75}). The major differences between PUMA
- and its predecessor SGCM are:
- \begin{itemize}
- \item The code is rewritten in portable
- FORTRAN-90 code, which removes problems associated with
- machine-specific properties like word lengths, floating point
- precision, output, etc. All the necessary routines are
- in the source code including the
- FFT ({\bf F}ast {\bf F}ourier {\bf T}ransformation)
- and the Legendre Transformation. The model can be run
- on any computer with a standard FORTRAN-90 compiler.
- The MPI-library is needed to run
- PUMA on parallel machines (see below).
- The Xlib (X11R6) library is needed for the graphical user
- interface.
- \item The
- truncation scheme is changed from the jagged triangular truncation
- to the standard triangular truncation scheme making it compatible to other
- T-models like ECHAM.
- \item The PUMA/Pumaburner system is data compatible to ECHAM/Afterburner.
- Thus all other ECHAM diagnostic software can be used on PUMA data.
- \item PUMA is fully parallelized and can use as many CPU's
- as half of the number of latitudes (e.g. 16 in T21 resolution). It uses the MPI
- ({\bf M}essage {\bf P}assing {\bf I}nterface) library while
- running on parallel systems or a cluster.
- MPI is not needed for running PUMA on a single CPU.
- \item The ongoing development added several new features like the preprocessor,
- graphical user interface, spherical harmonics mode selection, and many more.
- \end{itemize}
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