1 | subroutine calc_rayleigh |
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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 | ! Average the Rayleigh scattering in each band, weighting the |
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8 | ! average by the blackbody function at temperature tstellar. |
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9 | ! Works for an arbitrary mix of gases (currently CO2, N2 and |
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10 | ! H2 are possible). |
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11 | ! |
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12 | ! Authors |
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13 | ! ------- |
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14 | ! Robin Wordsworth (2010) |
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15 | ! Jeremy Leconte (2012): Added option for variable gas. Improved water rayleigh (Bucholtz 1995). |
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16 | ! Noé Clément (2022) : Additionnal comments & Methane+CO Rayleigh |
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17 | ! |
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18 | ! Called by |
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19 | ! --------- |
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20 | ! setspv.F |
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21 | ! |
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22 | ! Calls |
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23 | ! ----- |
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24 | ! none |
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25 | ! |
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26 | !================================================================== |
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27 | |
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28 | use radinc_h, only: L_NSPECTV |
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29 | use radcommon_h, only: WAVEV, BWNV, DWNV, tstellar, tauray, taurayvar, scalep |
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30 | use gases_h, only: ngasmx, vgas, gnom, gfrac, igas_CO2, igas_H2, & |
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31 | igas_H2O, igas_He, igas_N2, igas_CH4, igas_CO |
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32 | use comcstfi_mod, only: g, mugaz, pi |
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33 | |
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34 | implicit none |
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35 | |
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36 | real*8 wl |
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37 | integer N,Nfine,ifine,igas |
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38 | parameter(Nfine=500.0) |
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39 | real*8 :: P0 = 9.423D+6 ! Rayleigh scattering reference pressure in pascals. P0 = 93*101325 Pa |
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40 | |
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41 | logical typeknown |
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42 | real*8 tauvar,tauvarvar,tausum,tausumvar,tauwei,tauweivar,bwidth,bstart |
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43 | double precision df |
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44 | |
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45 | real*8 tauconsti(ngasmx) |
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46 | real*8 tauvari(ngasmx) |
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47 | |
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48 | integer icantbewrong |
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49 | |
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50 | ! we multiply by scalep here (100) because plev, which is used in optcv, |
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51 | ! is in units of mBar, so we need to convert. |
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52 | ! we calculate here TAURAY which is in m2/mBar |
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53 | |
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54 | ! tau0/p0=tau/p (Hansen 1974 : equation (2.31) ) |
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55 | ! Then calculate tau0 = (8*pi^3*p_1atm)/(3*N0^2) * 4*delta^2/(g*mugaz*lambda^4) (Hansen 1974 : equation (2.29) ) |
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56 | ! where delta=n-1 and N0 is an amagat |
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57 | |
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58 | ! In exo_k : (8*pi^3)/(3*N0^2) * 4 * delta^2 ------- is written : (24*pi^3)/(N0^2) * (4/9) * delta^2 |
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59 | |
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60 | ! (tauconsti * tauvari) = scalep * cross_section_molecule_exo_k / ( gravity * molecular_mass ) |
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61 | ! (tauconsti * tauvari) in m2/mBar because of scalep factor |
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62 | ! cross_section_molecule in m2/molecule |
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63 | ! molecular_mass is the mass of th considered molecule |
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64 | |
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65 | typeknown=.false. |
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66 | do igas=1,ngasmx |
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67 | if(igas.eq.vgas)then |
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68 | print*,'variable gas is ',trim(gnom(igas)),' in Rayleigh scattering ' |
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69 | endif |
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70 | if((igas/=vgas).and.(gfrac(igas).lt.5.e-2))then |
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71 | print*,'Ignoring ',trim(gnom(igas)),' in Rayleigh scattering '// & |
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72 | 'as its mixing ratio is less than 0.05.' |
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73 | ! ignore variable gas in Rayleigh calculation |
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74 | ! ignore gases of mixing ratio < 0.05 in Rayleigh calculation |
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75 | tauconsti(igas) = 0.0 |
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76 | else |
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77 | if(igas.eq.igas_CO2) then |
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78 | ! Hansen 1974 : equation (2.32) |
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79 | tauconsti(igas) = (8.7/g)*1.527*scalep/P0 |
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80 | elseif(igas.eq.igas_N2)then |
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81 | ! Hansen 1974 : equation (2.30) ---- (P0/93.0) is equal to 101325 Pa |
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82 | tauconsti(igas) = (9.81/g)*8.569E-3*scalep/(P0/93.0) |
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83 | elseif(igas.eq.igas_H2O)then |
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84 | ! tauconsti(igas) = (10.0/g)*9.22E-3*scalep/101325.0 |
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85 | tauconsti(igas) = 1.98017E-10*scalep/(g*mugaz*1E4) |
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86 | elseif(igas.eq.igas_H2)then |
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87 | tauconsti(igas) = (10.0/g)*0.0241*scalep/101325.0 |
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88 | ! tauconsti(igas) = (10.0/g)*0.0487*scalep/(101325.0) |
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89 | ! uses n=1.000132 from Optics, Fourth Edition. |
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90 | ! was out by a factor 2! |
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91 | |
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92 | ! below is exo_k formula : this tauconsti is consistent with commented tauvari for H2 below |
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93 | ! tauconsti(igas) = (1/(g*2.*1.6726*1E-27)) * 1E16 * scalep |
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94 | elseif(igas.eq.igas_He)then |
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95 | tauconsti(igas) = (10.0/g)*0.00086*scalep/101325.0 |
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96 | elseif(igas.eq.igas_CH4)then |
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97 | ! For CH4 we use the formalism of exo_k (developed by Jeremy Leconte) |
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98 | ! the relation between exo_k formalism and LMDZ formalism is : (tauconsti*tauvari)=scalep*sigma_exok/(gravity*molecular_mass) |
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99 | ! Values are taken from Caldas (2019), equation 12 & appendix D |
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100 | ! 24.*pi**3/(1E5/(1.380648813E-23*273.15))**2 is a constant |
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101 | ! 4/9=(2/3)**2 is approximately ((n+1)/(n**2+2))**2 |
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102 | ! 1E24 = (1E6)**4 because wavelength is in micron |
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103 | ! 16.04*1.6726*1E-27 is CH4 molecular mass |
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104 | tauconsti(igas) = 24.*pi**3/(1E5/(1.380648813E-23*273.15))**2 * 4./9. * 1E24 * (1/( g *16.04*1.6726*1E-27)) * scalep |
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105 | |
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106 | elseif(igas.eq.igas_CO)then |
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107 | ! see above for explanation |
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108 | ! 28.01*1.6726*1E-27 is CH4 molecular mass |
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109 | tauconsti(igas) = 24.*pi**3/(1E5/(1.380648813E-23*273.15))**2 * 4./9. * 1E24 * (1/( g *28.01*1.6726*1e-27)) * scalep |
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110 | else |
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111 | print*,'Error in calc_rayleigh: Gas species not recognised!' |
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112 | print*,"igas=",igas," gnom(igas)=",trim(gnom(igas)) |
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113 | call abort_physic("calc_rayleigh","Invalid gas",1) |
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114 | endif |
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115 | |
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116 | if((gfrac(igas).eq.1.0).and.(vgas.eq.0))then |
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117 | print*,'Rayleigh scattering is for a pure ',trim(gnom(igas)),' atmosphere.' |
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118 | typeknown=.true. |
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119 | endif |
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120 | |
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121 | endif |
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122 | enddo |
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123 | |
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124 | if(.not.typeknown)then |
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125 | print*,'Rayleigh scattering is for a mixed gas atmosphere.' |
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126 | typeknown=.true. |
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127 | endif |
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128 | |
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129 | |
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130 | do N=1,L_NSPECTV |
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131 | |
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132 | tausum = 0.0 |
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133 | tauwei = 0.0 |
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134 | tausumvar = 0.0 |
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135 | tauweivar = 0.0 |
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136 | bstart = 10000.0/BWNV(N+1) ! BWNV is in cm-1 so 10000.0/BWNV is in micron |
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137 | bwidth = (10000.0/BWNV(N)) - (10000.0/BWNV(N+1)) |
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138 | do ifine=1,Nfine |
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139 | wl=bstart+dble(ifine)*bwidth/Nfine |
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140 | |
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141 | tauvar=0.0 |
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142 | tauvarvar=0.0 |
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143 | do igas=1,ngasmx |
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144 | if((igas/=vgas).and.(gfrac(igas).lt.5.e-2))then |
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145 | ! ignore variable gas in Rayleigh calculation |
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146 | ! ignore gases of mixing ratio < 0.05 in Rayleigh calculation |
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147 | tauvari(igas) = 0.0 |
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148 | else |
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149 | if(igas.eq.igas_CO2)then |
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150 | tauvari(igas) = (1.0+0.013/wl**2)/wl**4 |
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151 | elseif(igas.eq.igas_N2)then |
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152 | tauvari(igas) = (1.0+0.0113/wl**2+0.00013/wl**4)/wl**4 |
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153 | elseif(igas.eq.igas_H2O)then |
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154 | ! tauvari(igas) = 1.0/wl**4 ! to be improved... |
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155 | tauvari(igas) = (5.7918E6/(2.38E2-1/wl**2)+1.679E5/(57.36E0-1/wl**2))**2/wl**4 |
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156 | elseif(igas.eq.igas_H2)then |
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157 | tauvari(igas) = 1.0/wl**4 |
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158 | |
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159 | ! below is exo_k formula : this tauvari is consistent with commented tauconsti for H2 above |
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160 | ! tauvari(igas) = (8.14E-49+1.28E-50/wl**2+1.61E-51/wl**4) / wl**4 |
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161 | elseif(igas.eq.igas_He)then |
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162 | tauvari(igas) = 1.0/wl**4 |
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163 | elseif(igas.eq.igas_CH4)then |
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164 | tauvari(igas) = (4.6662E-4+4.02E-6/wl**2)**2 / wl**4 |
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165 | elseif(igas.eq.igas_CO)then |
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166 | tauvari(igas) = (2.2851E-4 + 0.456E4/(5.101816E9 - 1E8/wl**2))**2 / wl**4 |
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167 | else |
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168 | print*,'Error in calc_rayleigh: Gas species not recognised!' |
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169 | call abort_physic("calc_rayleigh","Gas species not recognised",1) |
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170 | endif |
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171 | endif |
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172 | |
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173 | if(igas.eq.vgas) then |
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174 | tauvarvar=tauvarvar+tauconsti(igas)*tauvari(igas) |
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175 | tauvar=tauvar+0.0*0.0*gfrac(igas) |
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176 | else |
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177 | tauvar=tauvar+tauconsti(igas)*tauvari(igas)*gfrac(igas) |
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178 | endif |
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179 | |
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180 | enddo |
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181 | |
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182 | call blackl(dble(wl*1e-6),dble(tstellar),df) |
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183 | df=df*bwidth/Nfine |
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184 | tauwei=tauwei+df |
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185 | tausum=tausum+tauvar*df |
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186 | tauweivar=tauweivar+df |
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187 | tausumvar=tausumvar+tauvarvar*df |
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188 | |
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189 | enddo |
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190 | TAURAY(N)=tausum/tauwei |
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191 | TAURAYVAR(N)=tausumvar/tauweivar |
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192 | ! we multiply by scalep here (100) because plev, which is used in optcv, |
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193 | ! is in units of mBar, so we need to convert. |
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194 | |
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195 | end do |
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196 | |
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197 | IF (L_NSPECTV > 6) THEN |
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198 | icantbewrong = L_NSPECTV-6 |
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199 | print*,'At 1 atm and lambda = ',WAVEV(icantbewrong),' um' |
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200 | print*,'tau_R = ',TAURAY(icantbewrong)*1013.25 |
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201 | print*,'sig_R = ',TAURAY(icantbewrong)*g*mugaz*1.67e-27*100, & |
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202 | 'cm^2 molecule^-1' |
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203 | ENDIF |
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204 | |
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205 | end subroutine calc_rayleigh |
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