[1954] | 1 | \chapter{Zoomed simulations} |
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| 2 | |
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| 3 | \label{sc:zoom} |
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| 4 | |
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| 5 | The LMD GCM can use a zoom to enhance the resolution locally. |
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| 6 | In practice, one can |
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| 7 | increase the latitudinal resolution on the one hand, |
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| 8 | and the longitudinal resolution on |
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| 9 | the other hand. |
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| 10 | |
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| 11 | \section{To define the zoomed area} |
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| 12 | |
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| 13 | The zoom is defined in {\tt run.def}. |
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| 14 | Here are the variables that you want to set: |
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| 15 | |
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| 16 | \begin{itemize} |
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| 17 | \item East longitude (in degrees) of zoom center {\tt clon} |
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| 18 | \item latitude (in degrees) of zoom center {\tt clat} |
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| 19 | \item zooming factors, along longitude {\tt grossismx}. |
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| 20 | {\it Typically 1.5, 2 or even 3 (see below)} |
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| 21 | \item zooming factors, along latitude {\tt grossismy}. {\it Typically 1.5, 2 |
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| 22 | or even 3 (see below)} |
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| 23 | \item {\tt fxyhypb}: |
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| 24 | {\it {\bf must be set to "T" for a zoom}, whereas it must be F otherwise} |
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| 25 | \item extention in longitude of zoomed area {\tt dzoomx}. |
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| 26 | This is the total |
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| 27 | longitudinal extension of the zoomed region (degree). \newline |
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| 28 | {\it It is recommended that {\tt grossismx} $\times$ |
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| 29 | {\tt dzoomx} $< 200^o$} |
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| 30 | \item extention in latitude of the zoomed region {\tt dzoomy}. |
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| 31 | This is the total |
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| 32 | latitudinal extension of the zoomed region (degree). \newline |
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| 33 | {\it It is recommended that {\tt |
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| 34 | grossismy} $\times$ {\tt dzoomy} $< 100^o$} |
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| 35 | \item stiffness of the zoom along longitudes {\tt taux}. |
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| 36 | 2 is for a smooth transition in |
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| 37 | longitude, more means sharper transition. |
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| 38 | \item stiffness of the zoom along latitudes {\tt taux}. |
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| 39 | 2 is for a smooth transition in |
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| 40 | latitude, more means sharper transition. |
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| 41 | \end{itemize} |
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| 42 | |
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| 43 | \section{Making a zoomed initial state} |
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| 44 | |
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| 45 | One must start from an initial state archive {\tt start\_archive.nc} |
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| 46 | obtained from a previous |
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| 47 | simulation (see section~\ref{sc:newstart}) |
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| 48 | Then compile and run {\tt newstart.e} {\bf using the {\tt run.def} |
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| 49 | file designed for the zoom}. |
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| 50 | |
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| 51 | After running {\tt newstart.e}. The zoomed grid may be visualized |
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| 52 | using grads, for instance. |
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| 53 | Here is a grads script that can be used to map the grid above a topography |
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| 54 | map: |
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| 55 | |
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| 56 | \begin{verbatim} |
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| 57 | set mpdraw off |
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| 58 | set grid off |
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| 59 | sdfopen restart.nc |
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| 60 | set gxout grid |
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| 61 | set digsiz 0 |
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| 62 | set lon -180 180 |
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| 63 | d ps |
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| 64 | close 1 |
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| 65 | *** replace the path to surface.nc in the following line: |
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| 66 | sdfopen /u/forget/WWW/datagcm/datafile/surface.nc |
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| 67 | set lon -180 180 |
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| 68 | set gxout contour |
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| 69 | set clab off |
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| 70 | set cint 3 |
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| 71 | d zMOL |
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| 72 | \end{verbatim} |
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| 73 | |
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| 74 | |
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| 75 | \section{Running a zoomed simulation and stability issue} |
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| 76 | |
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| 77 | \begin{itemize} |
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| 78 | |
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| 79 | \item {\bf dynamical timestep} |
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| 80 | Because of their higher resolution, zoomed simulation requires a higher |
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| 81 | timestep. |
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| 82 | Therefore in {\tt run.def}, the number of dynamical timestep per day |
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| 83 | {\tt day\_step} must be increased by more than {\tt grossismx} or |
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| 84 | {\tt grossismy} (twice that if necessary). |
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| 85 | However, you can keep the same physical timestep (48/sol) and thus increase |
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| 86 | {\tt iphysiq} accordingly ({\tt iphysiq = day\_step/48}). |
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| 87 | |
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| 88 | %\item It has been found that when zooming in longitude, on must set |
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| 89 | %{\tt ngroup=1} in |
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| 90 | %{\tt dyn3d/groupeun.F}. Otherwise the run is less stable. |
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| 91 | |
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| 92 | \item The very first initial state made with {\tt newstart.e} can be noisy and |
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| 93 | dynamically unstable. |
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| 94 | It may be necessary to strongly increase the intensity of the |
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| 95 | dissipation and increase {\tt day\_step} in {\tt run.def} for 1 to 3 sols, |
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| 96 | and then use less strict values. |
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| 97 | |
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| 98 | \item If the run remains very unstable and requires too much dissipation |
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| 99 | or a too small timestep, a good tip to help stabilize the model |
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| 100 | is to decrease the vertical extension of your run and the number of |
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| 101 | layer (one generally zoom to study near-surface process, so 20 to 22 |
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| 102 | layers and a vertical extension up to 60 or 80 km is usually enough). |
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| 103 | |
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| 104 | \end{itemize} |
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