1 | MODULE optcv_mod |
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2 | |
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3 | IMPLICIT NONE |
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4 | |
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5 | CONTAINS |
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6 | |
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7 | SUBROUTINE OPTCV(DTAUV,TAUV,TAUCUMV,PLEV, & |
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8 | QXVAER,QSVAER,GVAER,WBARV,COSBV, & |
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9 | TAURAY,TAUAERO,TMID,PMID,TAUGSURF,QVAR,MUVAR) |
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10 | |
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11 | use radinc_h, only: L_NLAYRAD, L_NLEVRAD, L_LEVELS, L_NSPECTV, L_NGAUSS, L_REFVAR, NAERKIND |
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12 | use radcommon_h, only: gasv, tlimit, wrefVAR, Cmk, tgasref, pfgasref,wnov,scalep,indv,glat_ig |
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13 | use gases_h, only: gfrac, ngasmx, igas_H2, igas_H2O, igas_He, igas_N2, & |
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14 | igas_CH4, igas_CO2 |
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15 | use comcstfi_mod, only: g, r, mugaz |
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16 | use callkeys_mod, only: kastprof,continuum,graybody,callgasvis |
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17 | use recombin_corrk_mod, only: corrk_recombin, gasv_recomb |
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18 | use tpindex_mod, only: tpindex |
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19 | |
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20 | implicit none |
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21 | |
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22 | !================================================================== |
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23 | ! |
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24 | ! Purpose |
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25 | ! ------- |
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26 | ! Calculates shortwave optical constants at each level. |
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27 | ! |
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28 | ! Authors |
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29 | ! ------- |
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30 | ! Adapted from the NASA Ames code by R. Wordsworth (2009) |
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31 | ! |
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32 | !================================================================== |
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33 | ! |
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34 | ! THIS SUBROUTINE SETS THE OPTICAL CONSTANTS IN THE VISUAL |
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35 | ! IT CALCULATES FOR EACH LAYER, FOR EACH SPECTRAL INTERVAL IN THE VISUAL |
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36 | ! LAYER: WBAR, DTAU, COSBAR |
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37 | ! LEVEL: TAU |
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38 | ! |
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39 | ! TAUV(L,NW,NG) is the cumulative optical depth at the top of radiation code |
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40 | ! layer L. NW is spectral wavelength interval, ng the Gauss point index. |
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41 | ! |
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42 | ! TLEV(L) - Temperature at the layer boundary |
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43 | ! PLEV(L) - Pressure at the layer boundary (i.e. level) |
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44 | ! GASV(NT,NPS,NW,NG) - Visible k-coefficients |
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45 | ! |
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46 | !------------------------------------------------------------------- |
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47 | |
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48 | |
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49 | real*8,intent(out) :: DTAUV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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50 | real*8 DTAUKV(L_LEVELS,L_NSPECTV,L_NGAUSS) |
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51 | real*8,intent(out) :: TAUV(L_NLEVRAD,L_NSPECTV,L_NGAUSS) |
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52 | real*8,intent(out) :: TAUCUMV(L_LEVELS,L_NSPECTV,L_NGAUSS) |
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53 | real*8,intent(in) :: PLEV(L_LEVELS) |
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54 | real*8,intent(in) :: TMID(L_LEVELS), PMID(L_LEVELS) |
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55 | real*8,intent(out) :: COSBV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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56 | real*8,intent(out) :: WBARV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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57 | |
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58 | ! for aerosols |
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59 | real*8,intent(in) :: QXVAER(L_LEVELS,L_NSPECTV,NAERKIND) |
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60 | real*8,intent(in) :: QSVAER(L_LEVELS,L_NSPECTV,NAERKIND) |
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61 | real*8,intent(in) :: GVAER(L_LEVELS,L_NSPECTV,NAERKIND) |
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62 | real*8,intent(in) :: TAUAERO(L_LEVELS,NAERKIND) |
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63 | |
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64 | ! local arrays (saved for convenience as need be allocated) |
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65 | real*8,save,allocatable :: TAUAEROLK(:,:,:) |
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66 | real*8,save,allocatable :: TAEROS(:,:,:) |
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67 | !$OMP THREADPRIVATE(TAUAEROLK,TAEROS) |
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68 | |
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69 | integer L, NW, NG, K, LK, IAER |
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70 | integer MT(L_LEVELS), MP(L_LEVELS), NP(L_LEVELS) |
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71 | real*8 ANS, TAUGAS |
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72 | real*8,intent(in) :: TAURAY(L_NSPECTV) |
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73 | real*8 TRAY(L_LEVELS,L_NSPECTV) |
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74 | real*8 DPR(L_LEVELS), U(L_LEVELS) |
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75 | real*8 LCOEF(4), LKCOEF(L_LEVELS,4) |
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76 | |
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77 | real*8,intent(out) :: taugsurf(L_NSPECTV,L_NGAUSS-1) |
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78 | real*8 DCONT,DAERO |
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79 | real*8 DRAYAER |
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80 | double precision wn_cont, p_cont, p_air, T_cont, dtemp, dtempc |
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81 | double precision p_cross |
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82 | |
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83 | ! variable species mixing ratio variables |
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84 | real*8,intent(in) :: QVAR(L_LEVELS) |
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85 | real*8,intent(in) :: MUVAR(L_LEVELS) |
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86 | real*8 :: WRATIO(L_LEVELS) |
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87 | real*8 KCOEF(4) |
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88 | integer NVAR(L_LEVELS) |
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89 | |
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90 | ! temporary variables to reduce memory access time to gasv |
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91 | real*8 tmpk(2,2) |
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92 | real*8 tmpkvar(2,2,2) |
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93 | |
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94 | ! temporary variables for multiple aerosol calculation |
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95 | real*8 atemp(L_NLAYRAD,L_NSPECTV) |
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96 | real*8 btemp(L_NLAYRAD,L_NSPECTV) |
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97 | real*8 ctemp(L_NLAYRAD,L_NSPECTV) |
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98 | |
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99 | ! variables for k in units m^-1 |
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100 | real*8 dz(L_LEVELS) |
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101 | |
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102 | |
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103 | integer igas, jgas |
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104 | |
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105 | integer interm |
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106 | |
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107 | logical :: firstcall=.true. |
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108 | !$OMP THREADPRIVATE(firstcall) |
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109 | |
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110 | if (firstcall) then |
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111 | ! allocate local arrays of size "naerkind" (which are also |
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112 | ! "saved" so that this is done only once in for all even if |
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113 | ! we don't need to store the value from a time step to the next) |
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114 | allocate(TAUAEROLK(L_LEVELS,L_NSPECTV,NAERKIND)) |
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115 | allocate(TAEROS(L_LEVELS,L_NSPECTV,NAERKIND)) |
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116 | firstcall=.false. |
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117 | endif ! of if (firstcall) |
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118 | |
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119 | !! AS: to save time in computing continuum (see bilinearbig) |
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120 | IF (.not.ALLOCATED(indv)) THEN |
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121 | ALLOCATE(indv(L_NSPECTV,ngasmx,ngasmx)) |
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122 | indv = -9999 ! this initial value means "to be calculated" |
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123 | ENDIF |
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124 | |
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125 | !======================================================================= |
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126 | ! Determine the total gas opacity throughout the column, for each |
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127 | ! spectral interval, NW, and each Gauss point, NG. |
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128 | ! Calculate the continuum opacities, i.e., those that do not depend on |
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129 | ! NG, the Gauss index. |
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130 | |
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131 | taugsurf(:,:) = 0.0 |
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132 | dpr(:) = 0.0 |
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133 | lkcoef(:,:) = 0.0 |
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134 | |
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135 | do K=2,L_LEVELS |
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136 | DPR(k) = PLEV(K)-PLEV(K-1) |
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137 | |
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138 | ! if we have continuum opacities, we need dz |
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139 | if(kastprof)then |
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140 | dz(k) = dpr(k)*(1000.0d0*8.3145d0/muvar(k))*TMID(K)/(g*PMID(K)) |
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141 | U(k) = Cmk*DPR(k)*mugaz/muvar(k) |
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142 | else |
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143 | dz(k) = dpr(k)*R*TMID(K)/(glat_ig*PMID(K))*mugaz/muvar(k) |
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144 | U(k) = Cmk*DPR(k)*mugaz/muvar(k) ! only Cmk line in optci.F |
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145 | !JL13 the mugaz/muvar factor takes into account water meanmolecular weight if water is present |
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146 | endif |
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147 | |
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148 | call tpindex(PMID(K),TMID(K),QVAR(K),pfgasref,tgasref,WREFVAR, & |
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149 | LCOEF,MT(K),MP(K),NVAR(K),WRATIO(K)) |
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150 | |
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151 | do LK=1,4 |
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152 | LKCOEF(K,LK) = LCOEF(LK) |
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153 | end do |
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154 | end do ! levels |
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155 | |
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156 | ! Spectral dependance of aerosol absorption |
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157 | !JL18 It seems to be good to have aerosols in the first "radiative layer" of the gcm in the IR |
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158 | ! but visible does not handle very well diffusion in first layer. |
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159 | ! The tauaero and tauray are thus set to 0 (a small value for rayleigh because the code crashes otherwise) |
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160 | ! in the 4 first semilayers in optcv, but not optci. |
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161 | ! This solves random variations of the sw heating at the model top. |
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162 | do iaer=1,naerkind |
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163 | do NW=1,L_NSPECTV |
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164 | TAEROS(1:4,NW,IAER)=0.d0 |
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165 | do K=5,L_LEVELS |
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166 | TAEROS(K,NW,IAER) = TAUAERO(K,IAER) * QXVAER(K,NW,IAER) |
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167 | end do ! levels |
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168 | end do |
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169 | end do |
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170 | |
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171 | ! Rayleigh scattering |
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172 | do NW=1,L_NSPECTV |
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173 | TRAY(1:4,NW) = 1d-30 |
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174 | do K=5,L_LEVELS |
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175 | TRAY(K,NW) = TAURAY(NW) * DPR(K) |
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176 | end do ! levels |
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177 | end do |
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178 | |
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179 | ! we ignore K=1... |
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180 | do K=2,L_LEVELS |
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181 | |
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182 | do NW=1,L_NSPECTV |
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183 | |
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184 | DRAYAER = TRAY(K,NW) |
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185 | ! DRAYAER is Tau RAYleigh scattering, plus AERosol opacity |
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186 | do iaer=1,naerkind |
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187 | DRAYAER = DRAYAER + TAEROS(K,NW,IAER) |
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188 | end do |
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189 | |
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190 | DCONT = 0.0 ! continuum absorption |
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191 | |
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192 | if(continuum.and.(.not.graybody).and.callgasvis)then |
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193 | ! include continua if necessary |
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194 | wn_cont = dble(wnov(nw)) |
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195 | T_cont = dble(TMID(k)) |
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196 | do igas=1,ngasmx |
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197 | |
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198 | if(gfrac(igas).eq.-1)then ! variable |
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199 | p_cont = dble(PMID(k)*scalep*QVAR(k)) ! qvar = mol/mol |
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200 | else |
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201 | p_cont = dble(PMID(k)*scalep*gfrac(igas)*(1.-QVAR(k))) |
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202 | endif |
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203 | |
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204 | dtemp=0.0 |
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205 | if(igas.eq.igas_N2)then |
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206 | |
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207 | interm = indv(nw,igas,igas) |
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208 | ! call interpolateN2N2(wn_cont,T_cont,p_cont,dtemp,.false.,interm) |
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209 | indv(nw,igas,igas) = interm |
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210 | ! only goes to 500 cm^-1, so unless we're around a cold brown dwarf, this is irrelevant in the visible |
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211 | |
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212 | elseif(igas.eq.igas_H2)then |
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213 | |
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214 | ! first do self-induced absorption |
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215 | interm = indv(nw,igas,igas) |
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216 | call interpolateH2H2(wn_cont,T_cont,p_cont,dtemp,.false.,interm) |
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217 | indv(nw,igas,igas) = interm |
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218 | |
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219 | ! then cross-interactions with other gases |
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220 | do jgas=1,ngasmx |
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221 | p_cross = dble(PMID(k)*scalep*gfrac(jgas)*(1.-QVAR(k))) |
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222 | dtempc = 0.0 |
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223 | if(jgas.eq.igas_N2)then |
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224 | interm = indv(nw,igas,jgas) |
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225 | call interpolateN2H2(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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226 | indv(nw,igas,jgas) = interm |
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227 | ! should be irrelevant in the visible |
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228 | elseif(jgas.eq.igas_CO2)then |
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229 | interm = indv(nw,igas,jgas) |
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230 | call interpolateCO2H2(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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231 | indv(nw,igas,jgas) = interm |
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232 | ! might not be relevant in the visible |
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233 | elseif(jgas.eq.igas_He)then |
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234 | interm = indv(nw,igas,jgas) |
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235 | call interpolateH2He(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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236 | indv(nw,igas,jgas) = interm |
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237 | endif |
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238 | dtemp = dtemp + dtempc |
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239 | enddo |
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240 | |
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241 | elseif(igas.eq.igas_CH4)then |
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242 | |
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243 | ! first do self-induced absorption |
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244 | interm = indv(nw,igas,igas) |
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245 | call interpolateCH4CH4(wn_cont,T_cont,p_cont,dtemp,.false.,interm) |
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246 | indv(nw,igas,igas) = interm |
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247 | |
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248 | ! then cross-interactions with other gases |
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249 | do jgas=1,ngasmx |
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250 | p_cross = dble(PMID(k)*scalep*gfrac(jgas)*(1.-QVAR(k))) |
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251 | dtempc = 0.0d0 |
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252 | if(jgas.eq.igas_H2)then |
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253 | interm = indv(nw,igas,jgas) |
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254 | call interpolateH2CH4(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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255 | indv(nw,igas,jgas) = interm |
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256 | elseif(jgas.eq.igas_CO2)then |
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257 | interm = indv(nw,igas,jgas) |
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258 | call interpolateCO2CH4(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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259 | indv(nw,igas,jgas) = interm |
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260 | ! might not be relevant in the visible |
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261 | elseif(jgas.eq.igas_He)then |
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262 | interm = indv(nw,igas,jgas) |
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263 | call interpolateHeCH4(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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264 | indv(nw,igas,jgas) = interm |
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265 | endif |
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266 | dtemp = dtemp + dtempc |
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267 | enddo |
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268 | |
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269 | elseif(igas.eq.igas_H2O.and.T_cont.gt.100.0)then |
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270 | ! Compute self and foreign (with air) continuum of H2O |
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271 | p_air = dble(PMID(k)*scalep) - p_cont ! note assumes background is air! |
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272 | interm = indv(nw,igas,igas) |
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273 | call interpolateH2O_self_foreign(wn_cont,T_cont,p_cont,p_air,dtemp,.false.,interm) ! MTCKD v3.3 |
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274 | indv(nw,igas,igas) = interm |
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275 | |
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276 | endif |
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277 | |
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278 | DCONT = DCONT + dtemp |
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279 | |
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280 | enddo |
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281 | |
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282 | DCONT = DCONT*dz(k) |
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283 | |
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284 | endif |
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285 | |
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286 | do ng=1,L_NGAUSS-1 |
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287 | |
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288 | ! Now compute TAUGAS |
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289 | |
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290 | ! Interpolate between water mixing ratios |
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291 | ! WRATIO = 0.0 if the requested water amount is equal to, or outside the |
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292 | ! the water data range |
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293 | |
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294 | if(L_REFVAR.eq.1)then ! added by RW for special no variable case |
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295 | |
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296 | ! JVO 2017 : added tmpk because the repeated calls to gasi/v increased dramatically |
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297 | ! the execution time of optci/v -> ~ factor 2 on the whole radiative |
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298 | ! transfer on the tested simulations ! |
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299 | |
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300 | IF (corrk_recombin) THEN ! Added by JVO |
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301 | tmpk = GASV_RECOMB(MT(K):MT(K)+1,MP(K):MP(K)+1,1,NW,NG) ! contains the mix of recombined species |
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302 | ELSE |
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303 | tmpk = GASV(MT(K):MT(K)+1,MP(K):MP(K)+1,1,NW,NG) |
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304 | ENDIF |
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305 | |
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306 | KCOEF(1) = tmpk(1,1) ! KCOEF(1) = GASV(MT(K),MP(K),1,NW,NG) |
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307 | KCOEF(2) = tmpk(1,2) ! KCOEF(2) = GASV(MT(K),MP(K)+1,1,NW,NG) |
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308 | KCOEF(3) = tmpk(2,2) ! KCOEF(3) = GASV(MT(K)+1,MP(K)+1,1,NW,NG) |
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309 | KCOEF(4) = tmpk(2,1) ! KCOEF(4) = GASV(MT(K)+1,MP(K),1,NW,NG) |
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310 | |
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311 | else |
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312 | |
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313 | IF (corrk_recombin) THEN |
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314 | tmpkvar = GASV_RECOMB(MT(K):MT(K)+1,MP(K):MP(K)+1,NVAR(K):NVAR(K)+1,NW,NG) |
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315 | ELSE |
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316 | tmpkvar = GASV(MT(K):MT(K)+1,MP(K):MP(K)+1,NVAR(K):NVAR(K)+1,NW,NG) |
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317 | ENDIF |
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318 | |
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319 | KCOEF(1) = tmpkvar(1,1,1) + WRATIO(K) * & |
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320 | ( tmpkvar(1,1,2)-tmpkvar(1,1,1) ) |
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321 | |
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322 | KCOEF(2) = tmpkvar(1,2,1) + WRATIO(K) * & |
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323 | ( tmpkvar(1,2,2)-tmpkvar(1,2,1) ) |
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324 | |
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325 | KCOEF(3) = tmpkvar(2,2,1) + WRATIO(K) * & |
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326 | ( tmpkvar(2,2,2)-tmpkvar(2,2,1) ) |
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327 | |
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328 | KCOEF(4) = tmpkvar(2,1,1) + WRATIO(K) * & |
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329 | ( tmpkvar(2,1,2)-tmpkvar(2,1,1) ) |
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330 | |
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331 | |
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332 | endif |
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333 | |
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334 | ! Interpolate the gaseous k-coefficients to the requested T,P values |
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335 | |
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336 | ANS = LKCOEF(K,1)*KCOEF(1) + LKCOEF(K,2)*KCOEF(2) + & |
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337 | LKCOEF(K,3)*KCOEF(3) + LKCOEF(K,4)*KCOEF(4) |
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338 | |
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339 | TAUGAS = U(k)*ANS |
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340 | |
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341 | TAUGSURF(NW,NG) = TAUGSURF(NW,NG) + TAUGAS + DCONT |
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342 | DTAUKV(K,nw,ng) = TAUGAS & |
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343 | + DRAYAER & ! DRAYAER includes all scattering contributions |
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344 | + DCONT ! For parameterized continuum aborption |
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345 | |
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346 | end do |
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347 | |
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348 | ! Now fill in the "clear" part of the spectrum (NG = L_NGAUSS), |
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349 | ! which holds continuum opacity only |
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350 | |
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351 | NG = L_NGAUSS |
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352 | DTAUKV(K,nw,ng) = DRAYAER + DCONT ! Scattering + parameterized continuum absorption |
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353 | |
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354 | end do |
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355 | end do |
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356 | |
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357 | |
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358 | !======================================================================= |
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359 | ! Now the full treatment for the layers, where besides the opacity |
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360 | ! we need to calculate the scattering albedo and asymmetry factors |
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361 | |
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362 | !JL18 It seems to be good to have aerosols in the first "radiative layer" of the gcm in the IR |
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363 | ! but not in the visible |
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364 | ! The tauaero is thus set to 0 in the 4 first semilayers in optcv, but not optci. |
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365 | ! This solves random variations of the sw heating at the model top. |
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366 | do iaer=1,naerkind |
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367 | DO NW=1,L_NSPECTV |
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368 | TAUAEROLK(1:4,NW,IAER)=0.d0 |
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369 | DO K=5,L_LEVELS |
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370 | TAUAEROLK(K,NW,IAER) = TAUAERO(K,IAER) * QSVAER(K,NW,IAER) ! effect of scattering albedo |
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371 | ENDDO |
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372 | ENDDO |
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373 | end do |
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374 | |
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375 | DO NW=1,L_NSPECTV |
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376 | DO L=1,L_NLAYRAD-1 |
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377 | K = 2*L+1 |
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378 | atemp(L,NW) = SUM(GVAER(K,NW,1:naerkind) * TAUAEROLK(K,NW,1:naerkind))+SUM(GVAER(K+1,NW,1:naerkind) * TAUAEROLK(K+1,NW,1:naerkind)) |
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379 | btemp(L,NW) = SUM(TAUAEROLK(K,NW,1:naerkind)) + SUM(TAUAEROLK(K+1,NW,1:naerkind)) |
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380 | ctemp(L,NW) = btemp(L,NW) + 0.9999*(TRAY(K,NW) + TRAY(K+1,NW)) ! JVO 2017 : does this 0.999 is really meaningful ? |
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381 | btemp(L,NW) = btemp(L,NW) + TRAY(K,NW) + TRAY(K+1,NW) |
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382 | COSBV(L,NW,1:L_NGAUSS) = atemp(L,NW)/btemp(L,NW) |
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383 | END DO ! L vertical loop |
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384 | |
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385 | ! Last level |
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386 | L = L_NLAYRAD |
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387 | K = 2*L+1 |
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388 | atemp(L,NW) = SUM(GVAER(K,NW,1:naerkind) * TAUAEROLK(K,NW,1:naerkind)) |
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389 | btemp(L,NW) = SUM(TAUAEROLK(K,NW,1:naerkind)) |
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390 | ctemp(L,NW) = btemp(L,NW) + 0.9999*TRAY(K,NW) ! JVO 2017 : does this 0.999 is really meaningful ? |
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391 | btemp(L,NW) = btemp(L,NW) + TRAY(K,NW) |
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392 | COSBV(L,NW,1:L_NGAUSS) = atemp(L,NW)/btemp(L,NW) |
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393 | |
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394 | |
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395 | END DO ! NW spectral loop |
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396 | |
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397 | DO NG=1,L_NGAUSS |
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398 | DO NW=1,L_NSPECTV |
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399 | DO L=1,L_NLAYRAD-1 |
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400 | |
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401 | K = 2*L+1 |
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402 | DTAUV(L,nw,ng) = DTAUKV(K,NW,NG) + DTAUKV(K+1,NW,NG) |
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403 | WBARV(L,nw,ng) = ctemp(L,NW) / DTAUV(L,nw,ng) |
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404 | |
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405 | END DO ! L vertical loop |
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406 | |
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407 | ! Last level |
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408 | |
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409 | L = L_NLAYRAD |
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410 | K = 2*L+1 |
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411 | DTAUV(L,nw,ng) = DTAUKV(K,NW,NG) |
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412 | |
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413 | WBARV(L,NW,NG) = ctemp(L,NW) / DTAUV(L,NW,NG) |
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414 | |
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415 | END DO ! NW spectral loop |
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416 | END DO ! NG Gauss loop |
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417 | |
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418 | ! Total extinction optical depths |
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419 | |
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420 | DO NG=1,L_NGAUSS ! full gauss loop |
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421 | DO NW=1,L_NSPECTV |
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422 | TAUCUMV(1,NW,NG)=0.0D0 |
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423 | DO K=2,L_LEVELS |
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424 | TAUCUMV(K,NW,NG)=TAUCUMV(K-1,NW,NG)+DTAUKV(K,NW,NG) |
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425 | END DO |
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426 | |
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427 | DO L=1,L_NLAYRAD |
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428 | TAUV(L,NW,NG)=TAUCUMV(2*L,NW,NG) |
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429 | END DO |
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430 | TAUV(L,NW,NG)=TAUCUMV(2*L_NLAYRAD+1,NW,NG) |
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431 | END DO |
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432 | END DO ! end full gauss loop |
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433 | |
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434 | |
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435 | |
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436 | |
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437 | end subroutine optcv |
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438 | |
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439 | END MODULE optcv_mod |
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