1 | subroutine interpolateH2H2(wn,temp,pres,abcoef,firstcall) |
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2 | |
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3 | !================================================================== |
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4 | ! |
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5 | ! Purpose |
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6 | ! ------- |
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7 | ! Calculates the H2-H2 CIA opacity, using a lookup table from |
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8 | ! Borysow (2002) |
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9 | ! |
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10 | ! Authors |
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11 | ! ------- |
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12 | ! R. Wordsworth (2009) |
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13 | ! |
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14 | !================================================================== |
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15 | |
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16 | use datafile_mod, only: datadir |
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17 | implicit none |
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18 | |
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19 | ! input |
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20 | double precision wn ! wavenumber (cm^-1) |
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21 | double precision temp ! temperature (Kelvin) |
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22 | double precision pres ! pressure (Pascals) |
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23 | |
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24 | ! output |
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25 | double precision abcoef ! absorption coefficient (m^-1) |
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26 | |
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27 | integer nS,nT |
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28 | parameter(nS=1649) |
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29 | parameter(nT=14) |
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30 | |
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31 | double precision amagat |
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32 | double precision wn_arr(nS) |
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33 | double precision temp_arr(nT) |
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34 | double precision abs_arr(nS,nT) |
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35 | double precision data_tmp(nT/2+1) |
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36 | |
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37 | integer k |
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38 | logical firstcall |
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39 | |
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40 | save wn_arr, temp_arr, abs_arr |
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41 | |
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42 | character*100 dt_file |
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43 | integer strlen,ios |
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44 | |
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45 | amagat=(273.15/temp)*(pres/101325.0) |
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46 | |
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47 | if(firstcall)then |
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48 | |
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49 | ! 1.1 Open the ASCII files |
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50 | |
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51 | ! cold |
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52 | dt_file=TRIM(datadir)//'/continuum_data/H2H2_CIA_LT.dat' |
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53 | open(33,file=dt_file,form='formatted',status='old',iostat=ios) |
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54 | if (ios.ne.0) then ! file not found |
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55 | write(*,*) 'Error from interpolateH2H2' |
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56 | write(*,*) 'Data file ',trim(dt_file),' not found.' |
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57 | write(*,*)'Check that your path to datagcm:',trim(datadir) |
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58 | write(*,*)' is correct. You can change it in callphys.def with:' |
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59 | write(*,*)' datadir = /absolute/path/to/datagcm' |
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60 | write(*,*)' Also check that there is a continuum_data/H2H2_CIA_LT.dat there.' |
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61 | call abort |
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62 | else |
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63 | do k=1,nS |
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64 | read(33,*) data_tmp |
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65 | wn_arr(k)=data_tmp(1) |
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66 | abs_arr(k,1:7)=data_tmp(2:8) |
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67 | end do |
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68 | endif |
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69 | close(33) |
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70 | |
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71 | ! hot |
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72 | dt_file=TRIM(datadir)//'/continuum_data/H2H2_CIA_HT.dat' |
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73 | open(34,file=dt_file,form='formatted',status='old',iostat=ios) |
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74 | if (ios.ne.0) then ! file not found |
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75 | write(*,*) 'Error from interpolateH2H2' |
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76 | write(*,*) 'Data file ',trim(dt_file),' not found.' |
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77 | write(*,*)'Check that your path to datagcm:',trim(datadir) |
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78 | write(*,*)' is correct. You can change it in callphys.def with:' |
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79 | write(*,*)' datadir = /absolute/path/to/datagcm' |
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80 | write(*,*)' Also check that there is a continuum_data/H2H2_CIA_HT.dat there.' |
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81 | call abort |
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82 | else |
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83 | do k=1,nS |
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84 | read(34,*) data_tmp |
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85 | wn_arr(k)=data_tmp(1) |
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86 | ! wn_arr is identical |
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87 | abs_arr(k,8:14)=data_tmp(2:8) |
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88 | end do |
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89 | endif |
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90 | close(34) |
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91 | |
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92 | temp_arr(1) = 60. |
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93 | temp_arr(2) = 100. |
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94 | temp_arr(3) = 150. |
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95 | temp_arr(4) = 200. |
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96 | temp_arr(5) = 250. |
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97 | temp_arr(6) = 300. |
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98 | temp_arr(7) = 350. |
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99 | temp_arr(8) = 400. |
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100 | temp_arr(9) = 500. |
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101 | temp_arr(10) = 600. |
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102 | temp_arr(11) = 700. |
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103 | temp_arr(12) = 800. |
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104 | temp_arr(13) = 900. |
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105 | temp_arr(14) = 1000. |
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106 | |
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107 | |
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108 | print*,'interpolateH2H2: At wavenumber ',wn,' cm^-1' |
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109 | print*,' temperature ',temp,' K' |
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110 | print*,' pressure ',pres,' Pa' |
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111 | |
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112 | call bilinearH2H2(wn_arr,temp_arr,abs_arr,wn,temp,abcoef) |
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113 | |
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114 | print*,'the absorption is ',abcoef,' cm^-1 amg^-2' |
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115 | |
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116 | abcoef=abcoef*100.0*amagat**2 ! convert to m^-1 |
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117 | |
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118 | print*,'We have ',amagat,' amagats' |
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119 | print*,'So the absorption is ',abcoef,' m^-1' |
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120 | |
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121 | else |
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122 | |
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123 | call bilinearH2H2(wn_arr,temp_arr,abs_arr,wn,temp,abcoef) |
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124 | abcoef=abcoef*100.0*amagat**2 ! convert to m^-1 |
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125 | !print*,'The absorption is ',abcoef,' m^-1' |
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126 | |
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127 | ! unlike for Rayleigh scattering, we do not currently weight by the BB function |
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128 | ! however our bands are normally thin, so this is no big deal. |
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129 | |
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130 | endif |
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131 | |
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132 | return |
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133 | end subroutine interpolateH2H2 |
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134 | |
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135 | |
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136 | !------------------------------------------------------------------------- |
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137 | subroutine bilinearH2H2(x_arr,y_arr,f2d_arr,x_in,y_in,f) |
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138 | ! Necessary for interpolation of continuum data |
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139 | |
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140 | implicit none |
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141 | |
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142 | integer nX,nY,i,j,a,b |
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143 | parameter(nX=1649) |
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144 | parameter(nY=14) |
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145 | |
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146 | real*8 x_in,y_in,x,y,x1,x2,y1,y2 |
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147 | real*8 f,f11,f12,f21,f22,fA,fB |
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148 | real*8 x_arr(nX) |
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149 | real*8 y_arr(nY) |
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150 | real*8 f2d_arr(nX,nY) |
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151 | |
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152 | integer strlen |
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153 | character*100 label |
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154 | label='subroutine bilinear' |
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155 | |
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156 | x=x_in |
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157 | y=y_in |
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158 | |
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159 | ! 1st check we're within the wavenumber range |
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160 | if ((x.lt.x_arr(2)).or.(x.gt.x_arr(nX-2))) then |
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161 | f=0.0D+0 |
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162 | return |
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163 | else |
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164 | |
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165 | ! in the x (wavenumber) direction 1st |
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166 | i=1 |
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167 | 10 if (i.lt.(nX+1)) then |
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168 | if (x_arr(i).gt.x) then |
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169 | x1=x_arr(i-1) |
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170 | x2=x_arr(i) |
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171 | a=i-1 |
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172 | i=9999 |
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173 | endif |
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174 | i=i+1 |
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175 | goto 10 |
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176 | endif |
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177 | endif |
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178 | |
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179 | if ((y.lt.y_arr(1)).or.(y.gt.y_arr(nY))) then |
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180 | write(*,*) 'Warning from bilinearH2H2:' |
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181 | write(*,*) 'Outside continuum temperature range!' |
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182 | write(*,*) y,y_arr(1),y_arr(nY) |
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183 | if(y.lt.y_arr(1))then |
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184 | y=y_arr(1)+0.01 |
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185 | endif |
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186 | if(y.gt.y_arr(nY))then |
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187 | y=y_arr(nY)-0.01 |
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188 | endif |
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189 | endif |
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190 | !else |
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191 | |
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192 | ! in the y (temperature) direction 2nd |
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193 | j=1 |
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194 | 20 if (j.lt.(nY+1)) then |
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195 | if (y_arr(j).gt.y) then |
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196 | y1=y_arr(j-1) |
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197 | y2=y_arr(j) |
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198 | b=j-1 |
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199 | j=9999 |
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200 | endif |
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201 | j=j+1 |
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202 | goto 20 |
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203 | endif |
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204 | !endif |
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205 | |
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206 | f11=f2d_arr(a,b) |
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207 | f21=f2d_arr(a+1,b) |
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208 | f12=f2d_arr(a,b+1) |
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209 | f22=f2d_arr(a+1,b+1) |
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210 | |
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211 | ! 1st in x-direction |
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212 | fA=f11*(x2-x)/(x2-x1)+f21*(x-x1)/(x2-x1) |
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213 | fB=f12*(x2-x)/(x2-x1)+f22*(x-x1)/(x2-x1) |
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214 | |
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215 | ! then in y-direction |
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216 | f=fA*(y2-y)/(y2-y1)+fB*(y-y1)/(y2-y1) |
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217 | |
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218 | return |
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219 | end subroutine bilinearH2H2 |
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