1 | This directory contains source codes of utilities (programs) that can be |
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2 | used to process the LMD Mars GCM output files (like "diagfi" or |
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3 | "stats"). |
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4 | In addition most output file from one of these program can then be |
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5 | processed by another. |
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6 | |
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7 | See script "compile" for instructions and recommendations to compile |
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8 | the utilities. Once adequately modified, that script can be used to |
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9 | compile each utility; e.g. to build the zrecast.e utility program: |
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10 | > compile zrecast |
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11 | |
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12 | Note that inputs can be provided by (1) replying to questions on screen or |
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13 | (2) filling the corresponding *.def and redirecting the input of these *.def |
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14 | files instead. For example : |
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15 | > concatnc.e < concatnc.def |
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16 | > zrecast.e < zrecast.def |
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17 | |
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18 | -------------------------------------------------------------------- |
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19 | 1) concatnc.e : concatenate successive GCM output files |
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20 | -------------------------------------------------------------------- |
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21 | |
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22 | This program is used to concatenate consecutive |
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23 | output files ("diagfi", and even "stats") for a selection of |
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24 | variable, in order to obtain one single big file. The time dimension can |
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25 | be "sols" or "Ls" (in that last case, Ls will not be linear, and |
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26 | software like Grads may not be able to use it. To have a linear "Ls" |
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27 | timescale, you can use "Ls_Linear.e" (see below). |
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28 | You can also add a "Ls" variable corresponding solar longitude for each |
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29 | timestep by using the "adls" option. |
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30 | |
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31 | Output file is : concat.nc |
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32 | |
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33 | -------------------------------------------------------------------- |
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34 | 2) zrecast.e : put GCM data in physical vertical coordinate |
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35 | -------------------------------------------------------------------- |
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36 | |
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37 | GCM outputs are in GCM hybrid coordinate which do not correspond to any |
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38 | physical vertical coordinate ! zrecast is NECESSARY to make any publishable |
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39 | scientific figure. |
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40 | |
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41 | This program reads 4D (lon-lat-alt-time) fields from GCM output files |
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42 | (ie: diagfi.nc time series or concat.nc or stats.nc files) and, by |
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43 | integrating the hydrostatic equation, recasts data along the vertical |
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44 | direction. |
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45 | The vertical coordinate can be either 1) pressure, 2) above areoid |
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46 | altitudes, 3) above local surface altitudes or 4) distance to center of |
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47 | the planet. Some interpolation along the vertical direction is also |
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48 | done, following instructions given by user (levels may be specified |
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49 | or given as minimu,maximum and number of levels). |
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50 | For "above areoid altitudes" output, Atmospheric pressure is added to |
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51 | output dataset; for "pressure coordinate" outputs, the above areoid |
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52 | altitude of pressure is added to output dataset. |
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53 | |
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54 | Minimal requirements and dependencies: |
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55 | The dataset must include the following data: |
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56 | - surface pressure |
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57 | - atmospheric temperature |
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58 | - hybrid coordinates aps() and bps(), or sigma levels() |
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59 | - ground geopotential (in input file; if not found, it is sought |
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60 | in a 'diagfi.nc' file. If not found there, it is then sought in |
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61 | a 'phisinit.nc' file (see section 1.3.3 of program) |
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62 | |
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63 | - When integration the hydrostatic equation, we assume that R, the |
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64 | molecular Gas Constant, may not be constant, so it is computed as |
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65 | R=P/(rho*T) (P=Pressure, rho=density, T=temperature) |
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66 | If 'rho' is not available, then we use a constant R (see section |
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67 | 2.2 in source file) |
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68 | |
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69 | - Vertical interpolation : note that density (kg.m-3) and species density |
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70 | (e.g. in molecules.cm-3) must be vertically interpolated in log-space. For |
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71 | that purpose, these variables names must start with "rho" (exemple : rho for |
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72 | density, rho_co2, rho_o2, etc....) |
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73 | |
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74 | output file is : |
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75 | name_of_input_file_P.nc with pressure coordinate |
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76 | name_of_input_file_A.nc with altitude above areoid coordinate |
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77 | name_of_input_file_S.nc with altitude above local surface coordinate |
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78 | name_of_input_file_R.nc with altitude as distance to center of planet |
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79 | |
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80 | -------------------------------------------------------------------- |
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81 | 3) localtime.e : put GCM data in local time coordinate |
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82 | -------------------------------------------------------------------- |
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83 | |
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84 | Program to redistribute and interpolate the variable a the same |
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85 | local times everywhere (useful to mimic satellite observations, or |
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86 | analyse day to day variations at a given local time). |
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87 | input : diagfi.nc / concat.nc / stats.nc kind of files |
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88 | |
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89 | output file is : name_of_input_file_LT.nc |
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90 | |
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91 | -------------------------------------------------------------------- |
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92 | 4) lslin.e : redistribute and average gcm output in Ls coordinate. |
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93 | -------------------------------------------------------------------- |
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94 | |
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95 | This program has been designed to interpolate data in Solar Longitude (Ls) |
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96 | linear time coordinate (usable with grads) from Netcdf diagfi or concatnc |
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97 | files, and to average the instantaneous data in periodic Ls intervals |
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98 | (for comparison with binned dataset, for instance). |
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99 | |
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100 | lslin also creates a lslin.ctl file that can be read |
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101 | directly by grads (>xdfopen lsllin.ctl) to plot in Ls coordinate to |
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102 | avoid some problem with grads when grads think that "the time interval |
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103 | is too small"... |
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104 | |
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105 | Output file is : name_of_input_file_Ls.nc |
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106 | |
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107 | -------------------------------------------------------------------- |
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108 | 5) solzenangle.e : select GCM data at a given solar zenith angle |
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109 | -------------------------------------------------------------------- |
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110 | |
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111 | Program to redistribute and interpolate the variable a the same |
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112 | solar zenith angle (notably useful to mimic satellite observations and in particular |
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113 | SOLAR OCCULTATIONS by choosing solar zenith angle = 90°) |
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114 | The user choose between Morning and Evening side. |
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115 | |
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116 | input : diagfi.nc / concat.nc / stats.nc kind of files |
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117 | |
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118 | On the morning side output file (1 output per sol per grid point) is : |
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119 | name_of_input_file_MO.nc |
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120 | |
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121 | On the evening side output file is (1 output per sol per grid point): |
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122 | name_of_input_file_EV.nc |
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123 | |
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124 | -------------------------------------------------------------------- |
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125 | 6) hrecast.e : interpolate data at another horizontal grid resolution. |
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126 | -------------------------------------------------------------------- |
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127 | |
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128 | This program can interpolate GCM output on any horizontal grid (regular |
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129 | lat - lon) as long as it cover all the planet. |
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130 | The grid can be given points by points. The best way is to use the |
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131 | redirected input hrecast.def |
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132 | |
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133 | hrecast.e < hrecast.def |
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134 | |
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135 | |
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136 | -------------------------------------------------------------------- |
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137 | 7) expandstartfi.e : to plot data in a startfi.nc file |
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138 | -------------------------------------------------------------------- |
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139 | |
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140 | In startfi.nc file, data are not plotable because the horizontal coordinate |
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141 | in only a 1D list of all atmospheric columns on the planets. |
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142 | This program takes a physics start file ("startfi.nc") and recasts it |
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143 | on the corresponding lonxlat grid (so it contents may easily be displayed |
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144 | using Python, Grads, Ferret, etc.) |
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145 | |
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146 | Simply run expandstartfi.e as a command line with arguments: |
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147 | |
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148 | expandstartfi.e [infile.nc] [outfile.nc] |
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149 | |
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150 | (if infile is not specified, "startfi.nc" is used as default) |
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151 | (if outfile is not specified, it is built as "infile_ex.nc") |
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152 | |
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153 | -------------------------------------------------------------------- |
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154 | 8) extract.e : get data at specific coordinates for comparison with observations |
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155 | -------------------------------------------------------------------- |
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156 | |
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157 | This program extracts (ie: interpolates) pointwise values of an atmospheric |
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158 | variable from a 'zrecast'ed diagfi file (works if altitude is geometrical |
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159 | height or a pressure vertical coordinates) |
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160 | user has to specify: |
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161 | - name of input file |
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162 | - date (in sols) offset wrt the input file (e.g. if the input file "begins" |
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163 | at Ls=0, then the offset is 0; if the input file begins at Ls=30, the |
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164 | offset date corresponding to the first 3 months is 61+66+66=193 sols, etc.) |
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165 | - the "extraction mode": |
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166 | 1: extract individual values; user will specify values of |
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167 | lon lat alt Ls LT (all on a same line) |
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168 | on as many lines as there are sought values |
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169 | 2: extract a profile: user will specify on a first line the values of |
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170 | lon lat Ls LT (all on a same line) |
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171 | and then only specify values of altitudes (m or Pa depending on the |
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172 | coordinate in the input file), one per line, at which values are |
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173 | sought |
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174 | - output values are sent to (ASCII) output file 'infile_var_.dat', where |
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175 | 'infile' is the input file name (without trailing '.nc') and |
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176 | 'var' is the sought variable, for extraction mode 1 as |
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177 | lines of "lon lat alt Ls LT value" and for a profile (extraction mode 2) |
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178 | as lines of "alt value" |
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179 | |
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180 | NB: If there is no data to do an appropriate interpolation to extract |
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181 | the sought value, then a "missing_value" (taken from the variable's |
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182 | attribute in the input file, most likely -9.99E33) is returned. |
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183 | |
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184 | See files "extract.points.def" and "extract.profile.def" for examples of |
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185 | input format that would simply need to be redirected to extract.e, e.g.: |
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186 | |
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187 | extract.e < extract.points.def |
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188 | |
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189 | -------------------------------------------------------------------- |
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190 | 9) aeroptical.e : compute aerosol opacities at a given wavelength |
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191 | -------------------------------------------------------------------- |
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192 | |
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193 | Program to compute opacities [1/km] of all aerosols from dust, water ice, |
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194 | stormdust and topdust present in the input file, at a wavelength given by the user. |
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195 | Computation is made from the aerosol mass mixing ratios and effective radius, |
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196 | associated with air density (rho) and files containing the aerosol |
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197 | optical properties (generally present in the GCM datadir/ directory). |
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198 | The user have to precise the type of opacity : extinction or absorption. |
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199 | |
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200 | NB : water ice effective radius is known to be a bit inaccurate in the GCM, |
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201 | so reffwice can be prescribed by the user. |
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202 | |
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203 | input : diagfi.nc / concat.nc / stats.nc kind of files |
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204 | |
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205 | output file is : |
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206 | name_of_input_file_OPAext.nc for extinction opacities |
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207 | name_of_input_file_OPAabs.nc for absorption opacities |
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208 | |
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209 | aeroptical.e < aeroptical.def |
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