1 | SUBROUTINE OPTCV(DTAUV,TAUV,TAUCUMV,PLEV, & |
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2 | WBARV,COSBV,TAURAY,TMID,PMID,TAUGSURF) |
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3 | |
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4 | use radinc_h |
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5 | use radcommon_h, only: gasv, tlimit, Cmk, tgasref, pfgasref,wnov,scalep,indv,glat_ig,gweight |
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6 | use gases_h |
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7 | use comcstfi_mod, only: g, r |
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8 | use callkeys_mod, only: continuum,graybody,callgasvis |
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9 | |
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10 | implicit none |
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11 | |
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12 | !================================================================== |
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13 | ! |
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14 | ! Purpose |
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15 | ! ------- |
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16 | ! Calculates shortwave optical constants at each level. |
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17 | ! |
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18 | ! Authors |
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19 | ! ------- |
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20 | ! Adapted from the NASA Ames code by R. Wordsworth (2009) |
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21 | ! |
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22 | !================================================================== |
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23 | ! |
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24 | ! THIS SUBROUTINE SETS THE OPTICAL CONSTANTS IN THE VISUAL |
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25 | ! IT CALCULATES FOR EACH LAYER, FOR EACH SPECTRAL INTERVAL IN THE VISUAL |
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26 | ! LAYER: WBAR, DTAU, COSBAR |
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27 | ! LEVEL: TAU |
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28 | ! |
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29 | ! TAUV(L,NW,NG) is the cumulative optical depth at the top of radiation code |
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30 | ! layer L. NW is spectral wavelength interval, ng the Gauss point index. |
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31 | ! |
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32 | ! TLEV(L) - Temperature at the layer boundary |
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33 | ! PLEV(L) - Pressure at the layer boundary (i.e. level) |
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34 | ! GASV(NT,NPS,NW,NG) - Visible k-coefficients |
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35 | ! |
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36 | !------------------------------------------------------------------- |
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37 | |
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38 | |
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39 | real*8 DTAUV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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40 | real*8 DTAUKV(L_LEVELS,L_NSPECTV,L_NGAUSS) |
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41 | real*8 TAUV(L_NLEVRAD,L_NSPECTV,L_NGAUSS) |
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42 | real*8 TAUCUMV(L_LEVELS,L_NSPECTV,L_NGAUSS) |
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43 | real*8 PLEV(L_LEVELS) |
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44 | real*8 TMID(L_LEVELS), PMID(L_LEVELS) |
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45 | real*8 COSBV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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46 | real*8 WBARV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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47 | |
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48 | ! Titan customisation |
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49 | ! J. Vatant d'Ollone (2016) |
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50 | real*8 DHAZE_T(L_LEVELS,L_NSPECTI) |
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51 | real*8 DHAZES_T(L_LEVELS,L_NSPECTI) |
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52 | real*8 SSA_T(L_LEVELS,L_NSPECTI) |
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53 | real*8 ASF_T(L_LEVELS,L_NSPECTI) |
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54 | real*8 INT_DTAU(L_NLAYRAD,L_NSPECTI) |
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55 | real*8 K_HAZE(L_NLAYRAD,L_NSPECTI) |
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56 | |
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57 | CHARACTER*2 str2 |
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58 | ! ========================== |
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59 | |
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60 | integer L, NW, NG, K, LK, IAER |
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61 | integer MT(L_LEVELS), MP(L_LEVELS), NP(L_LEVELS) |
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62 | real*8 ANS, TAUGAS |
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63 | real*8 TAURAY(L_NSPECTV) |
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64 | real*8 TRAY(L_LEVELS,L_NSPECTV) |
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65 | real*8 DPR(L_LEVELS), U(L_LEVELS) |
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66 | real*8 LCOEF(4), LKCOEF(L_LEVELS,4) |
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67 | |
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68 | real*8 taugsurf(L_NSPECTV,L_NGAUSS-1) |
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69 | real*8 DCONT |
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70 | real*8 DRAYAER |
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71 | double precision wn_cont, p_cont, p_air, T_cont, dtemp, dtempc |
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72 | double precision p_cross |
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73 | |
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74 | real*8 KCOEF(4) |
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75 | |
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76 | ! temporary variable to reduce memory access time to gasv |
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77 | real*8 tmpk(2,2) |
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78 | |
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79 | ! temporary variables for multiple aerosol calculation |
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80 | real*8 atemp(L_NLAYRAD,L_NSPECTV) |
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81 | real*8 btemp(L_NLAYRAD,L_NSPECTV) |
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82 | real*8 ctemp(L_NLAYRAD,L_NSPECTV) |
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83 | |
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84 | ! variables for k in units m^-1 |
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85 | real*8 dz(L_LEVELS) |
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86 | |
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87 | integer igas, jgas, ilay |
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88 | |
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89 | integer interm |
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90 | |
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91 | !! AS: to save time in computing continuum (see bilinearbig) |
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92 | IF (.not.ALLOCATED(indv)) THEN |
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93 | ALLOCATE(indv(L_NSPECTV,ngasmx,ngasmx)) |
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94 | indv = -9999 ! this initial value means "to be calculated" |
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95 | ENDIF |
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96 | |
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97 | !======================================================================= |
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98 | ! Determine the total gas opacity throughout the column, for each |
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99 | ! spectral interval, NW, and each Gauss point, NG. |
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100 | ! Calculate the continuum opacities, i.e., those that do not depend on |
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101 | ! NG, the Gauss index. |
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102 | |
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103 | taugsurf(:,:) = 0.0 |
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104 | dpr(:) = 0.0 |
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105 | lkcoef(:,:) = 0.0 |
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106 | |
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107 | do K=2,L_LEVELS |
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108 | DPR(k) = PLEV(K)-PLEV(K-1) |
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109 | |
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110 | ! if we have continuum opacities, we need dz |
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111 | |
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112 | dz(k) = dpr(k)*R*TMID(K)/(glat_ig*PMID(K)) |
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113 | U(k) = Cmk*DPR(k) ! only Cmk line in optcv.F |
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114 | |
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115 | call tpindex(PMID(K),TMID(K),pfgasref,tgasref,LCOEF,MT(K),MP(K)) |
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116 | |
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117 | do LK=1,4 |
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118 | LKCOEF(K,LK) = LCOEF(LK) |
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119 | end do |
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120 | end do ! levels |
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121 | |
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122 | ! Rayleigh scattering |
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123 | do NW=1,L_NSPECTV |
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124 | do K=2,L_LEVELS |
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125 | TRAY(K,NW) = TAURAY(NW) * DPR(K) |
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126 | end do ! levels |
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127 | end do |
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128 | |
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129 | ! we ignore K=1... |
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130 | do K=2,L_LEVELS |
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131 | |
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132 | ilay = k / 2 ! int. arithmetic => gives the gcm layer index |
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133 | |
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134 | do NW=1,L_NSPECTV |
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135 | |
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136 | !================= Titan customisation ======================================== |
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137 | call disr_haze(dz(k),plev(k),wnov(nw),dhaze_T(k,nw),SSA_T(k,nw),ASF_T(k,nw)) |
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138 | ! ============================================================================= |
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139 | |
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140 | DRAYAER = TRAY(K,NW) |
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141 | ! DRAYAER is Tau RAYleigh scattering, plus AERosol opacity |
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142 | DRAYAER = DRAYAER + DHAZE_T(K,NW) ! Titan's aerosol |
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143 | |
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144 | DCONT = 0.0 ! continuum absorption |
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145 | |
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146 | if(continuum.and.(.not.graybody).and.callgasvis)then |
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147 | ! include continua if necessary |
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148 | wn_cont = dble(wnov(nw)) |
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149 | T_cont = dble(TMID(k)) |
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150 | do igas=1,ngasmx |
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151 | |
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152 | p_cont = dble(PMID(k)*scalep*gfrac(igas,ilay)) |
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153 | |
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154 | dtemp=0.0 |
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155 | if(igas.eq.igas_N2)then |
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156 | |
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157 | interm = indv(nw,igas,igas) |
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158 | ! call interpolateN2N2(wn_cont,T_cont,p_cont,dtemp,.false.,interm) |
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159 | indv(nw,igas,igas) = interm |
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160 | ! 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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161 | |
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162 | elseif(igas.eq.igas_H2)then |
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163 | |
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164 | ! first do self-induced absorption |
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165 | interm = indv(nw,igas,igas) |
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166 | call interpolateH2H2(wn_cont,T_cont,p_cont,dtemp,.false.,interm) |
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167 | indv(nw,igas,igas) = interm |
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168 | |
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169 | ! then cross-interactions with other gases |
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170 | do jgas=1,ngasmx |
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171 | p_cross = dble(PMID(k)*scalep*gfrac(jgas,ilay)) |
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172 | dtempc = 0.0 |
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173 | if(jgas.eq.igas_N2)then |
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174 | interm = indv(nw,igas,jgas) |
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175 | call interpolateN2H2(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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176 | indv(nw,igas,jgas) = interm |
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177 | ! should be irrelevant in the visible |
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178 | endif |
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179 | dtemp = dtemp + dtempc |
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180 | enddo |
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181 | |
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182 | elseif(igas.eq.igas_CH4)then |
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183 | |
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184 | ! first do self-induced absorption |
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185 | interm = indv(nw,igas,igas) |
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186 | call interpolateCH4CH4(wn_cont,T_cont,p_cont,dtemp,.false.,interm) |
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187 | indv(nw,igas,igas) = interm |
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188 | |
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189 | ! then cross-interactions with other gases |
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190 | do jgas=1,ngasmx |
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191 | p_cross = dble(PMID(k)*scalep*gfrac(jgas,ilay)) |
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192 | dtempc = 0.0 |
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193 | if(jgas.eq.igas_N2)then |
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194 | interm = indv(nw,igas,jgas) |
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195 | call interpolateN2CH4(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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196 | indv(nw,igas,jgas) = interm |
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197 | endif |
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198 | dtemp = dtemp + dtempc |
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199 | enddo |
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200 | |
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201 | endif |
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202 | |
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203 | DCONT = DCONT + dtemp |
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204 | |
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205 | enddo |
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206 | |
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207 | DCONT = DCONT*dz(k) |
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208 | |
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209 | endif |
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210 | |
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211 | do ng=1,L_NGAUSS-1 |
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212 | |
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213 | ! Now compute TAUGAS |
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214 | |
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215 | ! JVO 2017 : added tmpk because the repeated calls to gasi/v increased dramatically |
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216 | ! the execution time of optci/v -> ~ factor 2 on the whole radiative |
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217 | ! transfer on the tested simulations ! |
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218 | |
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219 | tmpk = GASV(MT(K):MT(K)+1,MP(K):MP(K)+1,1,NW,NG) |
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220 | |
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221 | KCOEF(1) = tmpk(1,1) ! KCOEF(1) = GASV(MT(K),MP(K),1,NW,NG) |
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222 | KCOEF(2) = tmpk(1,2) ! KCOEF(2) = GASV(MT(K),MP(K)+1,1,NW,NG) |
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223 | KCOEF(3) = tmpk(2,2) ! KCOEF(3) = GASV(MT(K)+1,MP(K)+1,1,NW,NG) |
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224 | KCOEF(4) = tmpk(2,1) ! KCOEF(4) = GASV(MT(K)+1,MP(K),1,NW,NG) |
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225 | |
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226 | ! Interpolate the gaseous k-coefficients to the requested T,P values |
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227 | |
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228 | ANS = LKCOEF(K,1)*KCOEF(1) + LKCOEF(K,2)*KCOEF(2) + & |
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229 | LKCOEF(K,3)*KCOEF(3) + LKCOEF(K,4)*KCOEF(4) |
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230 | |
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231 | |
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232 | TAUGAS = U(k)*ANS |
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233 | |
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234 | TAUGSURF(NW,NG) = TAUGSURF(NW,NG) + TAUGAS + DCONT |
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235 | DTAUKV(K,nw,ng) = TAUGAS & |
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236 | + DRAYAER & ! DRAYAER includes all scattering contributions |
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237 | + DCONT ! For parameterized continuum aborption |
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238 | |
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239 | end do |
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240 | |
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241 | ! Now fill in the "clear" part of the spectrum (NG = L_NGAUSS), |
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242 | ! which holds continuum opacity only |
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243 | |
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244 | NG = L_NGAUSS |
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245 | DTAUKV(K,nw,ng) = DRAYAER + DCONT ! Scattering + parameterized continuum absorption, including Titan's haze |
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246 | |
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247 | end do |
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248 | end do |
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249 | |
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250 | |
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251 | !======================================================================= |
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252 | ! Now the full treatment for the layers, where besides the opacity |
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253 | ! we need to calculate the scattering albedo and asymmetry factors |
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254 | |
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255 | ! Haze scattering |
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256 | DO NW=1,L_NSPECTV |
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257 | DO K=2,L_LEVELS |
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258 | DHAZES_T(K,NW) = DHAZE_T(K,NW) * SSA_T(K,NW) ! effect of scattering albedo on haze |
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259 | ENDDO |
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260 | ENDDO |
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261 | |
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262 | |
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263 | DO NW=1,L_NSPECTV |
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264 | DO L=1,L_NLAYRAD-1 |
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265 | K = 2*L+1 |
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266 | atemp(L,NW) = ASF_T(K,NW)*DHAZES_T(K,NW) + ASF_T(K+1,NW)*DHAZES_T(K+1,NW) |
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267 | btemp(L,NW) = DHAZES_T(K,NW) + DHAZES_T(K+1,NW) |
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268 | 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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269 | btemp(L,NW) = btemp(L,NW) + TRAY(K,NW) + TRAY(K+1,NW) |
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270 | COSBV(L,NW,1:L_NGAUSS) = atemp(L,NW)/btemp(L,NW) |
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271 | END DO ! L vertical loop |
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272 | |
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273 | ! Last level |
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274 | L = L_NLAYRAD |
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275 | K = 2*L+1 |
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276 | atemp(L,NW) = ASF_T(K,NW)*DHAZES_T(K,NW) |
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277 | btemp(L,NW) = DHAZES_T(K,NW) |
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278 | ctemp(L,NW) = btemp(L,NW) + 0.9999*TRAY(K,NW) ! JVO 2017 : does this 0.999 is really meaningful ? |
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279 | btemp(L,NW) = btemp(L,NW) + TRAY(K,NW) |
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280 | COSBV(L,NW,1:L_NGAUSS) = atemp(L,NW)/btemp(L,NW) |
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281 | |
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282 | |
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283 | END DO ! NW spectral loop |
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284 | |
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285 | DO NG=1,L_NGAUSS |
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286 | DO NW=1,L_NSPECTV |
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287 | DO L=1,L_NLAYRAD-1 |
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288 | |
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289 | K = 2*L+1 |
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290 | DTAUV(L,nw,ng) = DTAUKV(K,NW,NG) + DTAUKV(K+1,NW,NG) |
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291 | WBARV(L,nw,ng) = ctemp(L,NW) / DTAUV(L,nw,ng) |
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292 | |
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293 | END DO ! L vertical loop |
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294 | |
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295 | ! Last level |
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296 | |
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297 | L = L_NLAYRAD |
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298 | K = 2*L+1 |
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299 | DTAUV(L,nw,ng) = DTAUKV(K,NW,NG) |
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300 | |
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301 | WBARV(L,NW,NG) = ctemp(L,NW) / DTAUV(L,NW,NG) |
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302 | |
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303 | END DO ! NW spectral loop |
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304 | END DO ! NG Gauss loop |
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305 | |
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306 | ! Total extinction optical depths |
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307 | |
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308 | DO NG=1,L_NGAUSS ! full gauss loop |
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309 | DO NW=1,L_NSPECTV |
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310 | TAUV(1,NW,NG)=0.0D0 |
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311 | DO L=1,L_NLAYRAD |
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312 | TAUV(L+1,NW,NG)=TAUV(L,NW,NG)+DTAUV(L,NW,NG) |
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313 | END DO |
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314 | |
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315 | TAUCUMV(1,NW,NG)=0.0D0 |
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316 | DO K=2,L_LEVELS |
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317 | TAUCUMV(K,NW,NG)=TAUCUMV(K-1,NW,NG)+DTAUKV(K,NW,NG) |
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318 | END DO |
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319 | END DO |
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320 | END DO ! end full gauss loop |
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321 | |
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322 | |
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323 | ! Titan's outputs (JVO, 2016)=============================================== |
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324 | ! do l=1,L_NLAYRAD |
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325 | ! do nw=1,L_NSPECTV |
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326 | ! INT_DTAU(L,NW) = 0.0d+0 |
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327 | ! DO NG=1,L_NGAUSS |
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328 | ! INT_DTAU(L,NW)= INT_DTAU(L,NW) + dtauv(L,nw,ng)*gweight(NG) |
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329 | ! enddo |
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330 | ! enddo |
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331 | ! enddo |
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332 | |
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333 | ! do nw=1,L_NSPECTV |
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334 | ! write(str2,'(i2.2)') nw |
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335 | ! call writediagfi(1,'kgv'//str2,'Gaz extinction coefficient VI band '//str2,'m-1',1,int_dtau(L_NLAYRAD:1:-1,nw)/dz_lay(L_NLAYRAD:1:-1)) |
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336 | ! call writediagfi(1,'khv'//str2,'Haze extinction coefficient VI band '//str2,'m-1',1,k_haze(L_NLAYRAD:1:-1,nw)/dz_lay(L_NLAYRAD:1:-1)) |
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337 | ! enddo |
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338 | |
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339 | ! ============================================================================== |
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340 | |
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341 | |
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342 | return |
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343 | |
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344 | |
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345 | end subroutine optcv |
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