1 | !============================================================================== |
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2 | |
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3 | subroutine photolysis_online(nlayer, deutchem, nb_phot_max, |
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4 | $ alt, press, temp, mmean, |
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5 | $ i_co2, i_co, i_o, i_o1d, i_o2, i_o3, i_h, |
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6 | $ i_h2, i_oh, i_ho2, i_h2o2, i_h2o, |
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7 | $ i_n, i_n2d, i_no, i_no2, i_n2, nesp, rm, |
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8 | $ tau, sza, dist_sol, v_phot) |
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9 | |
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10 | use photolysis_mod |
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11 | |
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12 | implicit none |
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13 | |
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14 | ! input |
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15 | |
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16 | logical, intent(in) :: deutchem |
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17 | integer, intent(in) :: nesp ! total number of chemical species |
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18 | integer, intent(in) :: nlayer |
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19 | integer, intent(in) :: nb_phot_max |
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20 | integer, intent(in) :: i_co2, i_co, i_o, i_o1d, i_o2, i_o3, i_h, |
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21 | $ i_h2, i_oh, i_ho2, i_h2o2, i_h2o, |
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22 | $ i_n, i_n2d, i_no, i_no2, i_n2 |
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23 | |
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24 | real, dimension(nlayer), intent(in) :: press, temp, mmean ! pressure (hpa)/temperature (k)/mean molecular mass (g.mol-1) |
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25 | real, dimension(nlayer), intent(in) :: alt ! altitude (km) |
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26 | real, dimension(nlayer,nesp), intent(in) :: rm ! mixing ratios |
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27 | real, intent(in) :: tau ! integrated aerosol optical depth at the surface |
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28 | real, intent(in) :: sza ! solar zenith angle (degrees) |
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29 | real, intent(in) :: dist_sol ! solar distance (au) |
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30 | |
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31 | ! output |
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32 | |
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33 | real (kind = 8), dimension(nlayer,nb_phot_max) :: v_phot ! photolysis rates (s-1) |
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34 | |
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35 | ! solar flux at mars |
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36 | |
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37 | real, dimension(nw) :: fmars ! solar flux (w.m-2.nm-1) |
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38 | real :: factor |
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39 | |
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40 | ! cross-sections |
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41 | |
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42 | real, dimension(nlayer,nw,nphot) :: sj ! general cross-section array (cm2) |
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43 | |
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44 | ! atmosphere |
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45 | |
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46 | real, dimension(nlayer+1) :: zpress, zalt, ztemp, zmmean ! pressure (hpa)/altitude (km)/temperature (k)/mean molecular mass (g.mol-1) |
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47 | |
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48 | real, dimension(nlayer+1) :: colinc ! air column increment (molecule.cm-2) |
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49 | real, dimension(nlayer+1,nw) :: dtrl ! rayleigh optical depth |
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50 | real, dimension(nlayer+1,nw) :: dtaer ! aerosol optical depth |
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51 | real, dimension(nlayer+1,nw) :: omaer ! aerosol single scattering albedo |
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52 | real, dimension(nlayer+1,nw) :: gaer ! aerosol asymmetry parameter |
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53 | real, dimension(nlayer+1,nw) :: dtcld ! cloud optical depth |
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54 | real, dimension(nlayer+1,nw) :: omcld ! cloud single scattering albedo |
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55 | real, dimension(nlayer+1,nw) :: gcld ! cloud asymmetry parameter |
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56 | real, dimension(nlayer+1,nw,nabs) :: dtgas ! optical depth for each gas |
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57 | real, dimension(nlayer+1,nw) :: dagas ! total gas optical depth |
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58 | real, dimension(nlayer+1) :: edir, edn, eup ! normalised irradiances |
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59 | real, dimension(nlayer+1) :: fdir, fdn, fup ! normalised actinic fluxes |
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60 | real, dimension(nlayer+1) :: saflux ! total actinic flux |
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61 | |
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62 | integer, dimension(0:nlayer+1) :: nid |
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63 | real, dimension(0:nlayer+1,nlayer+1) :: dsdh |
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64 | |
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65 | integer :: j_o2_o, j_o2_o1d, j_co2_o, j_co2_o1d, j_o3_o1d, j_o3_o, |
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66 | $ j_h2o, j_h2o2, j_ho2, j_h2, j_no, j_no2, j_n2, |
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67 | $ j_hdo_od, j_hdo_d |
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68 | |
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69 | integer :: a_o2, a_co2, a_o3, a_h2o, a_h2o2, a_ho2, a_h2, a_no, |
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70 | $ a_no2, a_n2 |
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71 | integer :: nlev, i, ilay, ilev, iw, ialt |
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72 | real :: deltaj |
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73 | |
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74 | ! absorbing gas numbering |
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75 | |
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76 | a_o2 = 1 ! o2 |
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77 | a_co2 = 2 ! co2 |
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78 | a_o3 = 3 ! o3 |
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79 | a_h2o = 4 ! h2o |
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80 | a_h2o2 = 5 ! h2o2 |
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81 | a_ho2 = 6 ! ho2 |
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82 | a_h2 = 7 ! h2 |
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83 | a_no = 8 ! no |
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84 | a_no2 = 9 ! no2 |
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85 | a_n2 = 10 ! n2 |
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86 | |
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87 | ! photodissociation rates numbering. |
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88 | ! photodissociations must be ordered the same way in subroutine "indice" |
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89 | |
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90 | j_o2_o = 1 ! o2 + hv -> o + o |
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91 | j_o2_o1d = 2 ! o2 + hv -> o + o(1d) |
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92 | j_co2_o = 3 ! co2 + hv -> co + o |
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93 | j_co2_o1d = 4 ! co2 + hv -> co + o(1d) |
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94 | j_o3_o1d = 5 ! o3 + hv -> o2 + o(1d) |
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95 | j_o3_o = 6 ! o3 + hv -> o2 + o |
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96 | j_h2o = 7 ! h2o + hv -> h + oh |
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97 | j_h2o2 = 8 ! h2o2 + hv -> oh + oh |
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98 | j_ho2 = 9 ! ho2 + hv -> oh + o |
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99 | j_h2 = 10 ! h2 + hv -> h + h |
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100 | j_no = 11 ! no + hv -> n + o |
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101 | j_no2 = 12 ! no2 + hv -> no + o |
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102 | j_n2 = 13 ! n2 + hv -> n + n |
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103 | j_hdo_od = 14 ! hdo + hv -> od + h |
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104 | j_hdo_d = 15 ! hdo + hv -> d + oh |
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105 | |
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106 | !==== define working vertical grid for the uv radiative code |
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107 | |
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108 | nlev = nlayer + 1 |
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109 | |
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110 | do ilev = 1,nlev-1 |
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111 | zpress(ilev) = press(ilev) |
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112 | zalt(ilev) = alt(ilev) |
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113 | ztemp(ilev) = temp(ilev) |
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114 | zmmean(ilev) = mmean(ilev) |
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115 | end do |
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116 | |
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117 | zpress(nlev) = 0. ! top of the atmosphere |
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118 | zalt(nlev) = zalt(nlev-1) + (zalt(nlev-1) - zalt(nlev-2)) |
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119 | ztemp(nlev) = ztemp(nlev-1) |
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120 | zmmean(nlev) = zmmean(nlev-1) |
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121 | |
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122 | !==== air column increments and rayleigh optical depth |
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123 | |
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124 | call setair(nlev, nw, wl, wc, zpress, ztemp, zmmean, colinc, dtrl) |
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125 | |
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126 | !==== set temperature-dependent cross-sections and optical depths |
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127 | |
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128 | dtgas(:,:,:) = 0. |
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129 | |
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130 | ! o2: |
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131 | |
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132 | call seto2(nphot, nlayer, nw, wc, mopt, temp, xso2_150, xso2_200, |
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133 | $ xso2_250, xso2_300, yieldo2, j_o2_o, j_o2_o1d, |
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134 | $ colinc(1:nlayer), rm(:,i_o2), |
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135 | $ dtgas(1:nlayer,:,a_o2), sj) |
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136 | |
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137 | ! co2: |
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138 | |
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139 | call setco2(nphot, nlayer, nw, wc, temp, xsco2_195, xsco2_295, |
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140 | $ xsco2_370, yieldco2, j_co2_o, j_co2_o1d, |
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141 | $ colinc(1:nlayer), rm(:,i_co2), |
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142 | $ dtgas(1:nlayer,:,a_co2), sj) |
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143 | |
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144 | ! o3: |
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145 | |
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146 | call seto3(nphot, nlayer, nw, wc, temp, xso3_218, xso3_298, |
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147 | $ j_o3_o, j_o3_o1d, |
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148 | $ colinc(1:nlayer), rm(:,i_o3), |
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149 | $ dtgas(1:nlayer,:,a_o3), sj) |
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150 | |
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151 | ! h2o2: |
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152 | |
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153 | call seth2o2(nphot, nlayer, nw, wc, temp, xsh2o2, j_h2o2, |
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154 | $ colinc(1:nlayer), rm(:,i_h2o2), |
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155 | $ dtgas(1:nlayer,:,a_h2o2), sj) |
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156 | |
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157 | ! no2: |
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158 | |
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159 | call setno2(nphot, nlayer, nw, wc, temp, xsno2, xsno2_220, |
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160 | $ xsno2_294, yldno2_248, yldno2_298, j_no2, |
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161 | $ colinc(1:nlayer), rm(:,i_no2), |
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162 | $ dtgas(1:nlayer,:,a_no2), sj) |
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163 | |
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164 | !==== temperature-independent optical depths and cross-sections |
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165 | |
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166 | ! optical depths |
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167 | |
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168 | do ilay = 1,nlayer |
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169 | do iw = 1,nw-1 |
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170 | dtgas(ilay,iw,a_h2o) = colinc(ilay)*rm(ilay,i_h2o)*xsh2o(iw) |
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171 | dtgas(ilay,iw,a_ho2) = colinc(ilay)*rm(ilay,i_ho2)*xsho2(iw) |
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172 | dtgas(ilay,iw,a_h2) = colinc(ilay)*rm(ilay,i_h2)*xsh2(iw) |
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173 | dtgas(ilay,iw,a_no) = colinc(ilay)*rm(ilay,i_no)*xsno(iw) |
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174 | dtgas(ilay,iw,a_n2) = colinc(ilay)*rm(ilay,i_n2)*xsn2(iw) |
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175 | end do |
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176 | end do |
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177 | |
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178 | ! total gas optical depth |
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179 | |
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180 | dagas(:,:) = 0. |
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181 | |
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182 | do ilay = 1,nlayer |
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183 | do iw = 1,nw-1 |
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184 | do i = 1,nabs |
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185 | dagas(ilay,iw) = dagas(ilay,iw) + dtgas(ilay,iw,i) |
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186 | end do |
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187 | end do |
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188 | end do |
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189 | |
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190 | ! cross-sections |
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191 | |
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192 | do ilay = 1,nlayer |
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193 | do iw = 1,nw-1 |
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194 | sj(ilay,iw,j_h2o) = xsh2o(iw) ! h2o |
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195 | sj(ilay,iw,j_ho2) = xsho2(iw) ! ho2 |
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196 | sj(ilay,iw,j_h2) = xsh2(iw)*yieldh2(iw) ! h2 |
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197 | sj(ilay,iw,j_no) = xsno(iw)*yieldno(iw) ! no |
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198 | sj(ilay,iw,j_n2) = xsn2(iw)*yieldn2(iw) ! n2 |
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199 | end do |
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200 | end do |
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201 | |
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202 | ! if deuterium chemistry: hdo cross-section |
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203 | |
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204 | if (deutchem) then |
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205 | do ilay = 1,nlayer |
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206 | do iw = 1,nw-1 |
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207 | ! two chanels for hdo, with same cross-section |
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208 | sj(ilay,iw,j_hdo_od) = 0.5*xshdo(iw) ! hdo -> od + h |
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209 | sj(ilay,iw,j_hdo_d) = 0.5*xshdo(iw) ! hdo -> d + oh |
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210 | end do |
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211 | end do |
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212 | end if |
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213 | |
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214 | !==== set aerosol properties and optical depth |
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215 | |
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216 | call setaer(nlev,zalt,tau,nw,dtaer,omaer,gaer) |
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217 | |
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218 | !==== set cloud properties and optical depth |
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219 | |
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220 | call setcld(nlev,nw,dtcld,omcld,gcld) |
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221 | |
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222 | !==== slant path lengths in spherical geometry |
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223 | |
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224 | call sphers(nlev,zalt,sza,dsdh,nid) |
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225 | |
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226 | !==== solar flux at mars |
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227 | |
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228 | factor = (1./dist_sol)**2. |
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229 | do iw = 1,nw-1 |
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230 | fmars(iw) = f(iw)*factor |
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231 | end do |
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232 | |
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233 | !==== initialise photolysis rates |
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234 | |
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235 | v_phot(:,1:nphot) = 0. |
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236 | |
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237 | !==== start of wavelength lopp |
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238 | |
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239 | do iw = 1,nw-1 |
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240 | |
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241 | ! monochromatic radiative transfer. outputs are: |
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242 | ! normalized irradiances edir(nlev), edn(nlev), eup(nlev) |
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243 | ! normalized actinic fluxes fdir(nlev), fdn(nlev), fup(nlev) |
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244 | ! where |
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245 | ! dir = direct beam, dn = down-welling diffuse, up = up-welling diffuse |
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246 | |
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247 | call rtlink(nlev, nw, iw, albedo(iw), sza, dsdh, nid, dtrl, |
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248 | $ dagas, dtcld, omcld, gcld, dtaer, omaer, gaer, |
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249 | $ edir, edn, eup, fdir, fdn, fup) |
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250 | |
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251 | |
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252 | ! spherical actinic flux |
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253 | |
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254 | do ilay = 1,nlayer |
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255 | saflux(ilay) = fmars(iw)*(fdir(ilay) + fdn(ilay) + fup(ilay)) |
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256 | end do |
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257 | |
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258 | ! photolysis rate integration |
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259 | |
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260 | do i = 1,nphot |
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261 | do ilay = 1,nlayer |
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262 | deltaj = saflux(ilay)*sj(ilay,iw,i) |
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263 | v_phot(ilay,i) = v_phot(ilay,i) + deltaj*(wu(iw)-wl(iw)) |
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264 | end do |
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265 | end do |
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266 | |
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267 | ! eliminate small values |
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268 | |
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269 | where (v_phot(:,1:nphot) < 1.e-30) |
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270 | v_phot(:,1:nphot) = 0. |
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271 | end where |
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272 | |
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273 | end do ! iw |
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274 | |
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275 | contains |
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276 | |
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277 | !============================================================================== |
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278 | |
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279 | subroutine setair(nlev, nw, wl, wc, press, temp, zmmean, |
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280 | $ colinc, dtrl) |
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281 | |
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282 | *-----------------------------------------------------------------------------* |
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283 | *= PURPOSE: =* |
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284 | *= computes air column increments and rayleigh optical depth =* |
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285 | *-----------------------------------------------------------------------------* |
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286 | |
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287 | implicit none |
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288 | |
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289 | ! input: |
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290 | |
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291 | integer :: nlev, nw |
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292 | |
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293 | real, dimension(nw) :: wl, wc ! lower and central wavelength grid (nm) |
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294 | real, dimension(nlev) :: press, temp, zmmean ! pressure (hpa), temperature (k), molecular mass (g.mol-1) |
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295 | |
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296 | ! output: |
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297 | |
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298 | real, dimension(nlev) :: colinc ! air column increments (molecule.cm-2) |
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299 | real, dimension(nlev,nw) :: dtrl ! rayleigh optical depth |
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300 | |
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301 | ! local: |
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302 | |
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303 | real, parameter :: avo = 6.022e23 |
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304 | real, parameter :: g = 3.72 |
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305 | real :: dp, nu |
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306 | real, dimension(nw) :: srayl |
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307 | integer :: ilev, iw |
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308 | |
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309 | ! compute column increments |
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310 | |
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311 | do ilev = 1, nlev-1 |
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312 | dp = (press(ilev) - press(ilev+1))*100. |
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313 | colinc(ilev) = avo*0.1*dp/(zmmean(ilev)*g) |
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314 | end do |
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315 | colinc(nlev) = 0. |
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316 | |
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317 | do iw = 1, nw - 1 |
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318 | |
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319 | ! co2 rayleigh cross-section |
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320 | ! ityaksov et al., chem. phys. lett., 462, 31-34, 2008 |
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321 | |
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322 | nu = 1./(wc(iw)*1.e-7) |
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323 | srayl(iw) = 1.78e-26*nu**(4. + 0.625) |
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324 | srayl(iw) = srayl(iw)*1.e-20 ! cm2 |
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325 | |
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326 | do ilev = 1, nlev |
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327 | dtrl(ilev,iw) = colinc(ilev)*srayl(iw) ! cm2 |
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328 | end do |
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329 | end do |
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330 | |
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331 | end subroutine setair |
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332 | |
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333 | !============================================================================== |
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334 | |
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335 | subroutine setco2(nd, nlayer, nw, wc, tlay, xsco2_195, xsco2_295, |
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336 | $ xsco2_370, yieldco2, j_co2_o, j_co2_o1d, |
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337 | $ colinc, rm, dt, sj) |
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338 | |
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339 | !-----------------------------------------------------------------------------* |
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340 | != PURPOSE: =* |
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341 | != Set up the CO2 temperature-dependent cross-sections and optical depth =* |
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342 | !-----------------------------------------------------------------------------* |
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343 | |
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344 | implicit none |
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345 | |
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346 | ! input: |
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347 | |
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348 | integer :: nd ! number of photolysis rates |
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349 | integer :: nlayer ! number of vertical layers |
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350 | integer :: nw ! number of wavelength grid points |
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351 | integer :: j_co2_o, j_co2_o1d ! photolysis indexes |
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352 | real, dimension(nw) :: wc ! central wavelength for each interval |
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353 | real, dimension(nw) :: xsco2_195, xsco2_295, xsco2_370 ! co2 cross-sections (cm2) |
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354 | real, dimension(nw) :: yieldco2 ! co2 photodissociation yield |
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355 | real, dimension(nlayer) :: tlay ! temperature (k) |
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356 | real, dimension(nlayer) :: rm ! co2 mixing ratio |
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357 | real, dimension(nlayer) :: colinc ! air column increment (molecule.cm-2) |
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358 | |
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359 | ! output: |
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360 | |
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361 | real, dimension(nlayer,nw) :: dt ! optical depth |
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362 | real, dimension(nlayer,nw,nd) :: sj ! cross-section array (cm2) |
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363 | |
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364 | ! local: |
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365 | |
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366 | integer :: extrapol |
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367 | integer :: i, l |
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368 | real :: temp, sco2 |
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369 | |
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370 | ! extrapol = 0 no extrapolation below 195 k |
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371 | ! extrapol = 1 extrapolation below 195 k |
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372 | |
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373 | extrapol = 0 |
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374 | |
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375 | do i = 1, nlayer |
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376 | if (extrapol == 1) then |
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377 | temp = tlay(i) |
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378 | else |
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379 | temp = max(tlay(i), 195.) |
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380 | end if |
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381 | temp = min(temp, 370.) |
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382 | do l = 1, nw-1 |
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383 | if (temp <= 295.) then |
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384 | if (xsco2_195(l) /= 0. .and. xsco2_295(l) /= 0.) then |
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385 | sco2 = alog(xsco2_195(l)) |
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386 | $ + (alog(xsco2_295(l)) - alog(xsco2_195(l))) |
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387 | $ /(295. - 195.)*(temp - 195.) |
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388 | sco2 = exp(sco2) |
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389 | else |
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390 | sco2 = 0. |
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391 | end if |
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392 | else |
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393 | if (xsco2_295(l) /= 0. .and. xsco2_370(l) /= 0.) then |
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394 | sco2 = alog(xsco2_295(l)) |
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395 | $ + (alog(xsco2_370(l)) - alog(xsco2_295(l))) |
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396 | $ /(370. - 295.)*(temp - 295.) |
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397 | sco2 = exp(sco2) |
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398 | else |
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399 | sco2 = 0. |
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400 | end if |
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401 | end if |
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402 | |
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403 | ! optical depth |
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404 | |
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405 | dt(i,l) = colinc(i)*rm(i)*sco2 |
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406 | |
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407 | ! production of o(1d) for wavelengths shorter than 167 nm |
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408 | |
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409 | if (wc(l) >= 167.) then |
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410 | sj(i,l,j_co2_o) = sco2*yieldco2(l) |
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411 | sj(i,l,j_co2_o1d) = 0. |
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412 | else |
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413 | sj(i,l,j_co2_o) = 0. |
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414 | sj(i,l,j_co2_o1d) = sco2*yieldco2(l) |
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415 | end if |
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416 | end do |
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417 | end do |
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418 | |
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419 | end subroutine setco2 |
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420 | |
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421 | !============================================================================== |
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422 | |
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423 | subroutine seto2(nd, nlayer, nw, wc, mopt, tlay, xso2_150, |
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424 | $ xso2_200, xso2_250, xso2_300, yieldo2, j_o2_o, |
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425 | $ j_o2_o1d, colinc, rm, dt, sj) |
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426 | |
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427 | !-----------------------------------------------------------------------------* |
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428 | != PURPOSE: =* |
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429 | != Set up the O2 temperature-dependent cross-sections and optical depth =* |
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430 | !-----------------------------------------------------------------------------* |
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431 | |
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432 | implicit none |
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433 | |
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434 | ! input: |
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435 | |
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436 | integer :: nd ! number of photolysis rates |
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437 | integer :: nlayer ! number of vertical layers |
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438 | integer :: nw ! number of wavelength grid points |
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439 | integer :: mopt ! high-res/low-res switch |
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440 | integer :: j_o2_o, j_o2_o1d ! photolysis indexes |
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441 | real, dimension(nw) :: wc ! central wavelength for each interval |
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442 | real, dimension(nw) :: xso2_150, xso2_200, xso2_250, ! o2 cross-sections (cm2) |
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443 | $ xso2_300 |
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444 | real, dimension(nw) :: yieldo2 ! o2 photodissociation yield |
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445 | real, dimension(nlayer) :: tlay ! temperature (k) |
---|
446 | real, dimension(nlayer) :: rm ! o2 mixing ratio |
---|
447 | real, dimension(nlayer) :: colinc ! air column increment (molecule.cm-2) |
---|
448 | |
---|
449 | ! output: |
---|
450 | |
---|
451 | real, dimension(nlayer,nw) :: dt ! optical depth |
---|
452 | real, dimension(nlayer,nw,nd) :: sj ! cross-section array (cm2) |
---|
453 | |
---|
454 | ! local: |
---|
455 | |
---|
456 | integer :: ilev, iw |
---|
457 | real :: temp |
---|
458 | real :: xso2, factor |
---|
459 | |
---|
460 | ! correction by factor if low-resolution in schumann-runge bands |
---|
461 | |
---|
462 | if (mopt == 1) then |
---|
463 | factor = 1. |
---|
464 | else if (mopt == 2) then |
---|
465 | factor = 0.8 |
---|
466 | end if |
---|
467 | |
---|
468 | ! calculate temperature dependance |
---|
469 | |
---|
470 | do ilev = 1,nlayer |
---|
471 | temp = max(tlay(ilev),150.) |
---|
472 | temp = min(temp, 300.) |
---|
473 | do iw = 1, nw-1 |
---|
474 | if (tlay(ilev) > 250.) then |
---|
475 | xso2 = xso2_250(iw) + (xso2_300(iw) - xso2_250(iw)) |
---|
476 | $ /(300. - 250.)*(temp - 250.) |
---|
477 | else if (tlay(ilev) > 200.) then |
---|
478 | xso2 = xso2_200(iw) + (xso2_250(iw) - xso2_200(iw)) |
---|
479 | $ /(250. - 200.)*(temp - 200.) |
---|
480 | else |
---|
481 | xso2 = xso2_150(iw) + (xso2_200(iw) - xso2_150(iw)) |
---|
482 | $ /(200. - 150.)*(temp - 150.) |
---|
483 | end if |
---|
484 | |
---|
485 | if (wc(iw) > 180. .and. wc(iw) < 200.) then |
---|
486 | xso2 = xso2*factor |
---|
487 | end if |
---|
488 | |
---|
489 | ! optical depth |
---|
490 | |
---|
491 | dt(ilev,iw) = colinc(ilev)*rm(ilev)*xso2 |
---|
492 | |
---|
493 | ! production of o(1d) for wavelengths shorter than 175 nm |
---|
494 | |
---|
495 | if (wc(iw) >= 175.) then |
---|
496 | sj(ilev,iw,j_o2_o) = xso2*yieldo2(iw) |
---|
497 | sj(ilev,iw,j_o2_o1d) = 0. |
---|
498 | else |
---|
499 | sj(ilev,iw,j_o2_o) = 0. |
---|
500 | sj(ilev,iw,j_o2_o1d) = xso2*yieldo2(iw) |
---|
501 | end if |
---|
502 | |
---|
503 | end do |
---|
504 | end do |
---|
505 | |
---|
506 | end subroutine seto2 |
---|
507 | |
---|
508 | !============================================================================== |
---|
509 | |
---|
510 | subroutine seto3(nd, nlayer, nw, wc, tlay, xso3_218, xso3_298, |
---|
511 | $ j_o3_o, j_o3_o1d, |
---|
512 | $ colinc, rm, dt, sj) |
---|
513 | |
---|
514 | !-----------------------------------------------------------------------------* |
---|
515 | != PURPOSE: =* |
---|
516 | != Set up the O3 temperature dependent cross-sections and optical depth =* |
---|
517 | !-----------------------------------------------------------------------------* |
---|
518 | |
---|
519 | implicit none |
---|
520 | |
---|
521 | ! input: |
---|
522 | |
---|
523 | integer :: nd ! number of photolysis rates |
---|
524 | integer :: nlayer ! number of vertical layers |
---|
525 | integer :: nw ! number of wavelength grid points |
---|
526 | integer :: j_o3_o, j_o3_o1d ! photolysis indexes |
---|
527 | real, dimension(nw) :: wc ! central wavelength for each interval |
---|
528 | real, dimension(nw) :: xso3_218, xso3_298 ! o3 cross-sections (cm2) |
---|
529 | real, dimension(nlayer) :: tlay ! temperature (k) |
---|
530 | real, dimension(nlayer) :: rm ! o3 mixing ratio |
---|
531 | real, dimension(nlayer) :: colinc ! air column increment (molecule.cm-2) |
---|
532 | |
---|
533 | ! output: |
---|
534 | |
---|
535 | real, dimension(nlayer,nw) :: dt ! optical depth |
---|
536 | real, dimension(nlayer,nw,nd) :: sj ! cross-section array (cm2) |
---|
537 | |
---|
538 | ! local: |
---|
539 | ! |
---|
540 | integer :: ilev, iw |
---|
541 | real :: temp |
---|
542 | real, dimension(nw) :: xso3(nw) |
---|
543 | real, dimension(nw) :: qy1d ! quantum yield for o(1d) production |
---|
544 | real :: q1, q2, a1, a2, a3 |
---|
545 | |
---|
546 | do ilev = 1, nlayer |
---|
547 | temp = max(tlay(ilev), 218.) |
---|
548 | temp = min(temp,298.) |
---|
549 | do iw = 1, nw-1 |
---|
550 | xso3(iw) = xso3_218(iw) + (xso3_298(iw) - xso3_218(iw)) |
---|
551 | $ /(298. - 218.) *(temp - 218.) |
---|
552 | |
---|
553 | ! optical depth |
---|
554 | |
---|
555 | dt(ilev,iw) = colinc(ilev)*rm(ilev)*xso3(iw) |
---|
556 | |
---|
557 | end do |
---|
558 | |
---|
559 | ! calculate quantum yield for o(1d) production (jpl 2006) |
---|
560 | |
---|
561 | temp = max(tlay(ilev),200.) |
---|
562 | temp = min(temp,320.) |
---|
563 | do iw = 1, nw-1 |
---|
564 | if (wc(iw) <= 306.) then |
---|
565 | qy1d(iw) = 0.90 |
---|
566 | else if (wc(iw) > 306. .and. wc(iw) < 328.) then |
---|
567 | q1 = 1. |
---|
568 | q2 = exp(-825.518/(0.695*temp)) |
---|
569 | a1 = (304.225 - wc(iw))/5.576 |
---|
570 | a2 = (314.957 - wc(iw))/6.601 |
---|
571 | a3 = (310.737 - wc(iw))/2.187 |
---|
572 | qy1d(iw) = (q1/(q1 + q2))*0.8036*exp(-(a1*a1*a1*a1)) |
---|
573 | $ + (q2/(q1 + q2))*8.9061*(temp/300.)**2. |
---|
574 | $ *exp(-(a2*a2)) |
---|
575 | $ + 0.1192*(temp/300.)**1.5*exp(-(a3*a3)) |
---|
576 | $ + 0.0765 |
---|
577 | else if (wc(iw) >= 328. .and. wc(iw) <= 340.) then |
---|
578 | qy1d(iw) = 0.08 |
---|
579 | else |
---|
580 | qy1d(iw) = 0. |
---|
581 | endif |
---|
582 | end do |
---|
583 | do iw = 1, nw-1 |
---|
584 | sj(ilev,iw,j_o3_o) = xso3(iw)*(1. - qy1d(iw)) |
---|
585 | sj(ilev,iw,j_o3_o1d) = xso3(iw)*qy1d(iw) |
---|
586 | end do |
---|
587 | end do |
---|
588 | |
---|
589 | end subroutine seto3 |
---|
590 | |
---|
591 | !============================================================================== |
---|
592 | |
---|
593 | subroutine seth2o2(nd, nlayer, nw, wc, tlay, xsh2o2, j_h2o2, |
---|
594 | $ colinc, rm, dt, sj) |
---|
595 | |
---|
596 | !-----------------------------------------------------------------------------* |
---|
597 | != PURPOSE: =* |
---|
598 | != Set up the h2o2 temperature dependent cross-sections and optical depth =* |
---|
599 | !-----------------------------------------------------------------------------* |
---|
600 | |
---|
601 | implicit none |
---|
602 | |
---|
603 | ! input: |
---|
604 | |
---|
605 | integer :: nd ! number of photolysis rates |
---|
606 | integer :: nlayer ! number of vertical layers |
---|
607 | integer :: nw ! number of wavelength grid points |
---|
608 | integer :: j_h2o2 ! photolysis index |
---|
609 | real, dimension(nw) :: wc ! central wavelength for each interval |
---|
610 | real, dimension(nw) :: xsh2o2 ! h2o2 cross-sections (cm2) |
---|
611 | real, dimension(nlayer) :: tlay ! temperature (k) |
---|
612 | real, dimension(nlayer) :: rm ! h2o2 mixing ratio |
---|
613 | real, dimension(nlayer) :: colinc ! air column increment (molecule.cm-2) |
---|
614 | |
---|
615 | ! output: |
---|
616 | |
---|
617 | real, dimension(nlayer,nw) :: dt ! optical depth |
---|
618 | real, dimension(nlayer,nw,nd) :: sj ! cross-section array (cm2) |
---|
619 | |
---|
620 | ! local: |
---|
621 | |
---|
622 | integer :: ilev, iw |
---|
623 | real :: a0, a1, a2, a3, a4, a5, a6, a7 |
---|
624 | real :: b0, b1, b2, b3, b4 |
---|
625 | real :: lambda, suma, sumb, chi, temp, xs |
---|
626 | |
---|
627 | A0 = 6.4761E+04 |
---|
628 | A1 = -9.2170972E+02 |
---|
629 | A2 = 4.535649 |
---|
630 | A3 = -4.4589016E-03 |
---|
631 | A4 = -4.035101E-05 |
---|
632 | A5 = 1.6878206E-07 |
---|
633 | A6 = -2.652014E-10 |
---|
634 | A7 = 1.5534675E-13 |
---|
635 | |
---|
636 | B0 = 6.8123E+03 |
---|
637 | B1 = -5.1351E+01 |
---|
638 | B2 = 1.1522E-01 |
---|
639 | B3 = -3.0493E-05 |
---|
640 | B4 = -1.0924E-07 |
---|
641 | |
---|
642 | ! temperature dependance: jpl 2006 |
---|
643 | |
---|
644 | do ilev = 1,nlayer |
---|
645 | temp = min(max(tlay(ilev),200.),400.) |
---|
646 | chi = 1./(1. + exp(-1265./temp)) |
---|
647 | do iw = 1, nw-1 |
---|
648 | if ((wc(iw) >= 260.) .and. (wc(iw) < 350.)) then |
---|
649 | lambda = wc(iw) |
---|
650 | sumA = ((((((A7*lambda + A6)*lambda + A5)*lambda + |
---|
651 | $ A4)*lambda +A3)*lambda + A2)*lambda + |
---|
652 | $ A1)*lambda + A0 |
---|
653 | sumB = (((B4*lambda + B3)*lambda + B2)*lambda + |
---|
654 | $ B1)*lambda + B0 |
---|
655 | xs = (chi*sumA + (1. - chi)*sumB)*1.e-21 |
---|
656 | sj(ilev,iw,j_h2o2) = xs |
---|
657 | else |
---|
658 | sj(ilev,iw,j_h2o2) = xsh2o2(iw) |
---|
659 | end if |
---|
660 | |
---|
661 | ! optical depth |
---|
662 | |
---|
663 | dt(ilev,iw) = colinc(ilev)*rm(ilev)*sj(ilev,iw,j_h2o2) |
---|
664 | end do |
---|
665 | end do |
---|
666 | |
---|
667 | end subroutine seth2o2 |
---|
668 | |
---|
669 | !============================================================================== |
---|
670 | |
---|
671 | subroutine setno2(nd, nlayer, nw, wc, tlay, xsno2, xsno2_220, |
---|
672 | $ xsno2_294, yldno2_248, yldno2_298, j_no2, |
---|
673 | $ colinc, rm, dt, sj) |
---|
674 | |
---|
675 | !-----------------------------------------------------------------------------* |
---|
676 | != PURPOSE: =* |
---|
677 | != Set up the no2 temperature-dependent cross-sections and optical depth =* |
---|
678 | !-----------------------------------------------------------------------------* |
---|
679 | |
---|
680 | implicit none |
---|
681 | |
---|
682 | ! input: |
---|
683 | |
---|
684 | integer :: nd ! number of photolysis rates |
---|
685 | integer :: nlayer ! number of vertical layers |
---|
686 | integer :: nw ! number of wavelength grid points |
---|
687 | integer :: j_no2 ! photolysis index |
---|
688 | real, dimension(nw) :: wc ! central wavelength for each interval |
---|
689 | real, dimension(nw) :: xsno2, xsno2_220, xsno2_294 ! no2 absorption cross-section at 220-294 k (cm2) |
---|
690 | real, dimension(nw) :: yldno2_248, yldno2_298 ! no2 quantum yield at 248-298 k |
---|
691 | real, dimension(nlayer) :: tlay ! temperature (k) |
---|
692 | real, dimension(nlayer) :: rm ! no2 mixing ratio |
---|
693 | real, dimension(nlayer) :: colinc ! air column increment (molecule.cm-2) |
---|
694 | |
---|
695 | ! output: |
---|
696 | |
---|
697 | real, dimension(nlayer,nw) :: dt ! optical depth |
---|
698 | real, dimension(nlayer,nw,nd) :: sj ! cross-section array (cm2) |
---|
699 | |
---|
700 | ! local: |
---|
701 | |
---|
702 | integer :: ilev, iw |
---|
703 | real :: temp, qy |
---|
704 | |
---|
705 | ! temperature dependance: jpl 2006 |
---|
706 | |
---|
707 | do ilev = 1,nlayer |
---|
708 | temp = max(220.,min(tlay(ilev),294.)) |
---|
709 | do iw = 1, nw - 1 |
---|
710 | if (wc(iw) < 238.) then |
---|
711 | sj(ilev,iw,j_no2) = xsno2(iw) |
---|
712 | else |
---|
713 | sj(ilev,iw,j_no2) = xsno2_220(iw) |
---|
714 | $ + (xsno2_294(iw) - xsno2_220(iw)) |
---|
715 | $ /(294. - 220.)*(temp - 220.) |
---|
716 | end if |
---|
717 | |
---|
718 | ! optical depth |
---|
719 | |
---|
720 | dt(ilev,iw) = colinc(ilev)*rm(ilev)*sj(ilev,iw,j_no2) |
---|
721 | end do |
---|
722 | end do |
---|
723 | |
---|
724 | ! quantum yield: jpl 2006 |
---|
725 | |
---|
726 | do ilev = 1,nlayer |
---|
727 | temp = max(248.,min(tlay(ilev),298.)) |
---|
728 | do iw = 1, nw - 1 |
---|
729 | qy = yldno2_248(iw) + (yldno2_298(iw) - yldno2_248(iw)) |
---|
730 | $ /(298. - 248.)*(temp - 248.) |
---|
731 | sj(ilev,iw,j_no2) = sj(ilev,iw,j_no2)*qy |
---|
732 | end do |
---|
733 | end do |
---|
734 | |
---|
735 | end subroutine setno2 |
---|
736 | |
---|
737 | !============================================================================== |
---|
738 | |
---|
739 | subroutine setaer(nlev,zalt,tau,nw,dtaer,omaer,gaer) |
---|
740 | |
---|
741 | !-----------------------------------------------------------------------------* |
---|
742 | != PURPOSE: =* |
---|
743 | != Set aerosol properties for each specified altitude layer. Properties =* |
---|
744 | != may be wavelength dependent. =* |
---|
745 | !-----------------------------------------------------------------------------* |
---|
746 | |
---|
747 | implicit none |
---|
748 | |
---|
749 | ! input |
---|
750 | |
---|
751 | integer :: nlev ! number of vertical levels |
---|
752 | integer :: nw ! number of wavelength grid points |
---|
753 | real, dimension(nlev) :: zalt ! altitude (km) |
---|
754 | real :: tau ! integrated aerosol optical depth at the surface |
---|
755 | |
---|
756 | ! output |
---|
757 | |
---|
758 | real, dimension(nlev,nw) :: dtaer ! aerosol optical depth |
---|
759 | real, dimension(nlev,nw) :: omaer ! aerosol single scattering albedo |
---|
760 | real, dimension(nlev,nw) :: gaer ! aerosol asymmetry parameter |
---|
761 | |
---|
762 | ! local |
---|
763 | |
---|
764 | integer :: ilev, iw |
---|
765 | real, dimension(nlev) :: aer ! dust extinction |
---|
766 | real :: omega, g, scaleh, gamma |
---|
767 | real :: dz, tautot, q0 |
---|
768 | |
---|
769 | omega = 0.622 ! single scattering albedo : wolff et al.(2010) at 258 nm |
---|
770 | g = 0.88 ! asymmetry factor : mateshvili et al. (2007) at 210 nm |
---|
771 | scaleh = 10. ! scale height (km) |
---|
772 | gamma = 0.03 ! conrath parameter |
---|
773 | |
---|
774 | dtaer(:,:) = 0. |
---|
775 | omaer(:,:) = 0. |
---|
776 | gaer(:,:) = 0. |
---|
777 | |
---|
778 | ! optical depth profile: |
---|
779 | |
---|
780 | tautot = 0. |
---|
781 | do ilev = 1, nlev-1 |
---|
782 | dz = zalt(ilev+1) - zalt(ilev) |
---|
783 | tautot = tautot + exp(gamma*(1. - exp(zalt(ilev)/scaleh)))*dz |
---|
784 | end do |
---|
785 | |
---|
786 | q0 = tau/tautot |
---|
787 | do ilev = 1, nlev-1 |
---|
788 | dz = zalt(ilev+1) - zalt(ilev) |
---|
789 | dtaer(ilev,:) = q0*exp(gamma*(1. - exp(zalt(ilev)/scaleh)))*dz |
---|
790 | omaer(ilev,:) = omega |
---|
791 | gaer(ilev,:) = g |
---|
792 | end do |
---|
793 | |
---|
794 | end subroutine setaer |
---|
795 | |
---|
796 | !============================================================================== |
---|
797 | |
---|
798 | subroutine setcld(nlev,nw,dtcld,omcld,gcld) |
---|
799 | |
---|
800 | !-----------------------------------------------------------------------------* |
---|
801 | != PURPOSE: =* |
---|
802 | != Set cloud properties for each specified altitude layer. Properties =* |
---|
803 | != may be wavelength dependent. =* |
---|
804 | !-----------------------------------------------------------------------------* |
---|
805 | |
---|
806 | implicit none |
---|
807 | |
---|
808 | ! input |
---|
809 | |
---|
810 | integer :: nlev ! number of vertical levels |
---|
811 | integer :: nw ! number of wavelength grid points |
---|
812 | |
---|
813 | ! output |
---|
814 | |
---|
815 | real, dimension(nlev,nw) :: dtcld ! cloud optical depth |
---|
816 | real, dimension(nlev,nw) :: omcld ! cloud single scattering albedo |
---|
817 | real, dimension(nlev,nw) :: gcld ! cloud asymmetry parameter |
---|
818 | |
---|
819 | ! local |
---|
820 | |
---|
821 | integer :: ilev, iw |
---|
822 | |
---|
823 | ! dtcld : optical depth |
---|
824 | ! omcld : single scattering albedo |
---|
825 | ! gcld : asymmetry factor |
---|
826 | |
---|
827 | dtcld(:,:) = 0. |
---|
828 | |
---|
829 | do ilev = 1,nlev-1 |
---|
830 | do iw = 1,nw-1 |
---|
831 | dtcld(ilev,iw) = 0. ! no clouds for the moment |
---|
832 | omcld(ilev,iw) = 0.99 |
---|
833 | gcld(ilev,iw) = 0.85 |
---|
834 | end do |
---|
835 | end do |
---|
836 | |
---|
837 | end subroutine setcld |
---|
838 | |
---|
839 | !============================================================================== |
---|
840 | |
---|
841 | subroutine sphers(nlev, z, zen, dsdh, nid) |
---|
842 | |
---|
843 | !-----------------------------------------------------------------------------* |
---|
844 | != PURPOSE: =* |
---|
845 | != Calculate slant path over vertical depth ds/dh in spherical geometry. =* |
---|
846 | != Calculation is based on: A.Dahlback, and K.Stamnes, A new spheric model =* |
---|
847 | != for computing the radiation field available for photolysis and heating =* |
---|
848 | != at twilight, Planet.Space Sci., v39, n5, pp. 671-683, 1991 (Appendix B) =* |
---|
849 | !-----------------------------------------------------------------------------* |
---|
850 | != PARAMETERS: =* |
---|
851 | != NZ - INTEGER, number of specified altitude levels in the working (I)=* |
---|
852 | != grid =* |
---|
853 | != Z - REAL, specified altitude working grid (km) (I)=* |
---|
854 | != ZEN - REAL, solar zenith angle (degrees) (I)=* |
---|
855 | != DSDH - REAL, slant path of direct beam through each layer crossed (O)=* |
---|
856 | != when travelling from the top of the atmosphere to layer i; =* |
---|
857 | != DSDH(i,j), i = 0..NZ-1, j = 1..NZ-1 =* |
---|
858 | != NID - INTEGER, number of layers crossed by the direct beam when (O)=* |
---|
859 | != travelling from the top of the atmosphere to layer i; =* |
---|
860 | != NID(i), i = 0..NZ-1 =* |
---|
861 | !-----------------------------------------------------------------------------* |
---|
862 | |
---|
863 | implicit none |
---|
864 | |
---|
865 | ! input |
---|
866 | |
---|
867 | integer, intent(in) :: nlev |
---|
868 | real, dimension(nlev), intent(in) :: z |
---|
869 | real, intent(in) :: zen |
---|
870 | |
---|
871 | ! output |
---|
872 | |
---|
873 | INTEGER nid(0:nlev) |
---|
874 | REAL dsdh(0:nlev,nlev) |
---|
875 | |
---|
876 | ! more program constants |
---|
877 | |
---|
878 | REAL re, ze(nlev) |
---|
879 | REAL dr |
---|
880 | real radius |
---|
881 | parameter (radius = 3393.) |
---|
882 | |
---|
883 | ! local |
---|
884 | |
---|
885 | real :: pi, zenrad, rpsinz, rj, rjp1, dsj, dhj, ga, gb, sm |
---|
886 | integer :: i, j, k, id, nlay |
---|
887 | |
---|
888 | REAL zd(0:nlev-1) |
---|
889 | |
---|
890 | !----------------------------------------------------------------------------- |
---|
891 | |
---|
892 | pi = acos(-1.0) |
---|
893 | dr = pi/180. |
---|
894 | zenrad = zen*dr |
---|
895 | |
---|
896 | ! number of layers: |
---|
897 | |
---|
898 | nlay = nlev - 1 |
---|
899 | |
---|
900 | ! include the elevation above sea level to the radius of Mars: |
---|
901 | |
---|
902 | re = radius + z(1) |
---|
903 | |
---|
904 | ! correspondingly z changed to the elevation above Mars surface: |
---|
905 | |
---|
906 | DO k = 1, nlev |
---|
907 | ze(k) = z(k) - z(1) |
---|
908 | END DO |
---|
909 | |
---|
910 | ! inverse coordinate of z |
---|
911 | |
---|
912 | zd(0) = ze(nlev) |
---|
913 | DO k = 1, nlay |
---|
914 | zd(k) = ze(nlev - k) |
---|
915 | END DO |
---|
916 | |
---|
917 | ! initialise dsdh(i,j), nid(i) |
---|
918 | |
---|
919 | nid(:) = 0. |
---|
920 | dsdh(:,:) = 0. |
---|
921 | |
---|
922 | ! calculate ds/dh of every layer |
---|
923 | |
---|
924 | do i = 0,nlay |
---|
925 | rpsinz = (re + zd(i))*sin(zenrad) |
---|
926 | |
---|
927 | IF ( (zen .GT. 90.0) .AND. (rpsinz .LT. re) ) THEN |
---|
928 | nid(i) = -1 |
---|
929 | ELSE |
---|
930 | |
---|
931 | ! Find index of layer in which the screening height lies |
---|
932 | |
---|
933 | id = i |
---|
934 | if (zen > 90.) then |
---|
935 | do j = 1,nlay |
---|
936 | IF( (rpsinz .LT. ( zd(j-1) + re ) ) .AND. |
---|
937 | $ (rpsinz .GE. ( zd(j) + re )) ) id = j |
---|
938 | end do |
---|
939 | end if |
---|
940 | |
---|
941 | do j = 1,id |
---|
942 | sm = 1.0 |
---|
943 | IF (j .EQ. id .AND. id .EQ. i .AND. zen .GT. 90.0) |
---|
944 | $ sm = -1.0 |
---|
945 | |
---|
946 | rj = re + zd(j-1) |
---|
947 | rjp1 = re + zd(j) |
---|
948 | |
---|
949 | dhj = zd(j-1) - zd(j) |
---|
950 | |
---|
951 | ga = rj*rj - rpsinz*rpsinz |
---|
952 | gb = rjp1*rjp1 - rpsinz*rpsinz |
---|
953 | |
---|
954 | ga = max(ga, 0.) |
---|
955 | gb = max(gb, 0.) |
---|
956 | |
---|
957 | IF (id.GT.i .AND. j.EQ.id) THEN |
---|
958 | dsj = sqrt(ga) |
---|
959 | ELSE |
---|
960 | dsj = sqrt(ga) - sm*sqrt(gb) |
---|
961 | END IF |
---|
962 | dsdh(i,j) = dsj/dhj |
---|
963 | end do |
---|
964 | nid(i) = id |
---|
965 | end if |
---|
966 | end do ! i = 0,nlay |
---|
967 | |
---|
968 | end subroutine sphers |
---|
969 | |
---|
970 | !============================================================================== |
---|
971 | |
---|
972 | SUBROUTINE rtlink(nlev, nw, iw, ag, zen, dsdh, nid, dtrl, |
---|
973 | $ dagas, dtcld, omcld, gcld, dtaer, omaer, gaer, |
---|
974 | $ edir, edn, eup, fdir, fdn, fup) |
---|
975 | |
---|
976 | implicit none |
---|
977 | |
---|
978 | ! input |
---|
979 | |
---|
980 | integer, intent(in) :: nlev, nw, iw ! number of wavelength grid points |
---|
981 | REAL ag |
---|
982 | REAL zen |
---|
983 | REAL dsdh(0:nlev,nlev) |
---|
984 | INTEGER nid(0:nlev) |
---|
985 | |
---|
986 | REAL dtrl(nlev,nw) |
---|
987 | REAL dagas(nlev,nw) |
---|
988 | REAL dtcld(nlev,nw), omcld(nlev,nw), gcld(nlev,nw) |
---|
989 | REAL dtaer(nlev,nw), omaer(nlev,nw), gaer(nlev,nw) |
---|
990 | |
---|
991 | ! output |
---|
992 | |
---|
993 | REAL edir(nlev), edn(nlev), eup(nlev) |
---|
994 | REAL fdir(nlev), fdn(nlev), fup(nlev) |
---|
995 | |
---|
996 | ! local: |
---|
997 | |
---|
998 | REAL dt(nlev), om(nlev), g(nlev) |
---|
999 | REAL dtabs,dtsct,dscld,dsaer,dacld,daaer |
---|
1000 | INTEGER i, ii |
---|
1001 | real, parameter :: largest = 1.e+36 |
---|
1002 | |
---|
1003 | ! specific two ps2str |
---|
1004 | |
---|
1005 | REAL ediri(nlev), edni(nlev), eupi(nlev) |
---|
1006 | REAL fdiri(nlev), fdni(nlev), fupi(nlev) |
---|
1007 | |
---|
1008 | logical, save :: delta = .true. |
---|
1009 | |
---|
1010 | !$OMP THREADPRIVATE(delta) |
---|
1011 | |
---|
1012 | !_______________________________________________________________________ |
---|
1013 | |
---|
1014 | ! initialize: |
---|
1015 | |
---|
1016 | do i = 1, nlev |
---|
1017 | fdir(i) = 0. |
---|
1018 | fup(i) = 0. |
---|
1019 | fdn(i) = 0. |
---|
1020 | edir(i) = 0. |
---|
1021 | eup(i) = 0. |
---|
1022 | edn(i) = 0. |
---|
1023 | end do |
---|
1024 | |
---|
1025 | do i = 1, nlev - 1 |
---|
1026 | dscld = dtcld(i,iw)*omcld(i,iw) |
---|
1027 | dacld = dtcld(i,iw)*(1.-omcld(i,iw)) |
---|
1028 | |
---|
1029 | dsaer = dtaer(i,iw)*omaer(i,iw) |
---|
1030 | daaer = dtaer(i,iw)*(1.-omaer(i,iw)) |
---|
1031 | |
---|
1032 | dtsct = dtrl(i,iw) + dscld + dsaer |
---|
1033 | dtabs = dagas(i,iw) + dacld + daaer |
---|
1034 | |
---|
1035 | dtabs = amax1(dtabs,1./largest) |
---|
1036 | dtsct = amax1(dtsct,1./largest) |
---|
1037 | |
---|
1038 | ! invert z-coordinate: |
---|
1039 | |
---|
1040 | ii = nlev - i |
---|
1041 | dt(ii) = dtsct + dtabs |
---|
1042 | om(ii) = dtsct/(dtsct + dtabs) |
---|
1043 | IF(dtsct .EQ. 1./largest) om(ii) = 1./largest |
---|
1044 | g(ii) = (gcld(i,iw)*dscld + |
---|
1045 | $ gaer(i,iw)*dsaer)/dtsct |
---|
1046 | end do |
---|
1047 | |
---|
1048 | ! call rt routine: |
---|
1049 | |
---|
1050 | call ps2str(nlev, zen, ag, dt, om, g, |
---|
1051 | $ dsdh, nid, delta, |
---|
1052 | $ fdiri, fupi, fdni, ediri, eupi, edni) |
---|
1053 | |
---|
1054 | ! output (invert z-coordinate) |
---|
1055 | |
---|
1056 | do i = 1, nlev |
---|
1057 | ii = nlev - i + 1 |
---|
1058 | fdir(i) = fdiri(ii) |
---|
1059 | fup(i) = fupi(ii) |
---|
1060 | fdn(i) = fdni(ii) |
---|
1061 | edir(i) = ediri(ii) |
---|
1062 | eup(i) = eupi(ii) |
---|
1063 | edn(i) = edni(ii) |
---|
1064 | end do |
---|
1065 | |
---|
1066 | end subroutine rtlink |
---|
1067 | |
---|
1068 | *=============================================================================* |
---|
1069 | |
---|
1070 | subroutine ps2str(nlev,zen,rsfc,tauu,omu,gu, |
---|
1071 | $ dsdh, nid, delta, |
---|
1072 | $ fdr, fup, fdn, edr, eup, edn) |
---|
1073 | |
---|
1074 | !-----------------------------------------------------------------------------* |
---|
1075 | != PURPOSE: =* |
---|
1076 | != Solve two-stream equations for multiple layers. The subroutine is based =* |
---|
1077 | != on equations from: Toon et al., J.Geophys.Res., v94 (D13), Nov 20, 1989.=* |
---|
1078 | != It contains 9 two-stream methods to choose from. A pseudo-spherical =* |
---|
1079 | != correction has also been added. =* |
---|
1080 | !-----------------------------------------------------------------------------* |
---|
1081 | != PARAMETERS: =* |
---|
1082 | != NLEVEL - INTEGER, number of specified altitude levels in the working (I)=* |
---|
1083 | != grid =* |
---|
1084 | != ZEN - REAL, solar zenith angle (degrees) (I)=* |
---|
1085 | != RSFC - REAL, surface albedo at current wavelength (I)=* |
---|
1086 | != TAUU - REAL, unscaled optical depth of each layer (I)=* |
---|
1087 | != OMU - REAL, unscaled single scattering albedo of each layer (I)=* |
---|
1088 | != GU - REAL, unscaled asymmetry parameter of each layer (I)=* |
---|
1089 | != DSDH - REAL, slant path of direct beam through each layer crossed (I)=* |
---|
1090 | != when travelling from the top of the atmosphere to layer i; =* |
---|
1091 | != DSDH(i,j), i = 0..NZ-1, j = 1..NZ-1 =* |
---|
1092 | != NID - INTEGER, number of layers crossed by the direct beam when (I)=* |
---|
1093 | != travelling from the top of the atmosphere to layer i; =* |
---|
1094 | != NID(i), i = 0..NZ-1 =* |
---|
1095 | != DELTA - LOGICAL, switch to use delta-scaling (I)=* |
---|
1096 | != .TRUE. -> apply delta-scaling =* |
---|
1097 | != .FALSE.-> do not apply delta-scaling =* |
---|
1098 | != FDR - REAL, contribution of the direct component to the total (O)=* |
---|
1099 | != actinic flux at each altitude level =* |
---|
1100 | != FUP - REAL, contribution of the diffuse upwelling component to (O)=* |
---|
1101 | != the total actinic flux at each altitude level =* |
---|
1102 | != FDN - REAL, contribution of the diffuse downwelling component to (O)=* |
---|
1103 | != the total actinic flux at each altitude level =* |
---|
1104 | != EDR - REAL, contribution of the direct component to the total (O)=* |
---|
1105 | != spectral irradiance at each altitude level =* |
---|
1106 | != EUP - REAL, contribution of the diffuse upwelling component to (O)=* |
---|
1107 | != the total spectral irradiance at each altitude level =* |
---|
1108 | != EDN - REAL, contribution of the diffuse downwelling component to (O)=* |
---|
1109 | *= the total spectral irradiance at each altitude level =* |
---|
1110 | !-----------------------------------------------------------------------------* |
---|
1111 | |
---|
1112 | implicit none |
---|
1113 | |
---|
1114 | ! input: |
---|
1115 | |
---|
1116 | INTEGER nlev |
---|
1117 | REAL zen, rsfc |
---|
1118 | REAL tauu(nlev), omu(nlev), gu(nlev) |
---|
1119 | REAL dsdh(0:nlev,nlev) |
---|
1120 | INTEGER nid(0:nlev) |
---|
1121 | LOGICAL delta |
---|
1122 | |
---|
1123 | ! output: |
---|
1124 | |
---|
1125 | REAL fup(nlev),fdn(nlev),fdr(nlev) |
---|
1126 | REAL eup(nlev),edn(nlev),edr(nlev) |
---|
1127 | |
---|
1128 | ! local: |
---|
1129 | |
---|
1130 | REAL tausla(0:nlev), tauc(0:nlev) |
---|
1131 | REAL mu2(0:nlev), mu, sum |
---|
1132 | |
---|
1133 | ! internal coefficients and matrix |
---|
1134 | |
---|
1135 | REAL lam(nlev),taun(nlev),bgam(nlev) |
---|
1136 | REAL e1(nlev),e2(nlev),e3(nlev),e4(nlev) |
---|
1137 | REAL cup(nlev),cdn(nlev),cuptn(nlev),cdntn(nlev) |
---|
1138 | REAL mu1(nlev) |
---|
1139 | INTEGER row |
---|
1140 | REAL a(2*nlev),b(2*nlev),d(2*nlev),e(2*nlev),y(2*nlev) |
---|
1141 | |
---|
1142 | ! other: |
---|
1143 | |
---|
1144 | REAL pifs, fdn0 |
---|
1145 | REAL gi(nlev), omi(nlev), tempg |
---|
1146 | REAL f, g, om |
---|
1147 | REAL gam1, gam2, gam3, gam4 |
---|
1148 | real, parameter :: largest = 1.e+36 |
---|
1149 | real, parameter :: precis = 1.e-7 |
---|
1150 | |
---|
1151 | ! For calculations of Associated Legendre Polynomials for GAMA1,2,3,4 |
---|
1152 | ! in delta-function, modified quadrature, hemispheric constant, |
---|
1153 | ! Hybrid modified Eddington-delta function metods, p633,Table1. |
---|
1154 | ! W.E.Meador and W.R.Weaver, GAS,1980,v37,p.630 |
---|
1155 | ! W.J.Wiscombe and G.W. Grams, GAS,1976,v33,p2440, |
---|
1156 | ! uncomment the following two lines and the appropriate statements further |
---|
1157 | ! down. |
---|
1158 | ! REAL YLM0, YLM2, YLM4, YLM6, YLM8, YLM10, YLM12, YLMS, BETA0, |
---|
1159 | ! > BETA1, BETAn, amu1, subd |
---|
1160 | |
---|
1161 | REAL expon, expon0, expon1, divisr, temp, up, dn |
---|
1162 | REAL ssfc |
---|
1163 | INTEGER nlayer, mrows, lev |
---|
1164 | |
---|
1165 | INTEGER i, j |
---|
1166 | |
---|
1167 | ! Some additional program constants: |
---|
1168 | |
---|
1169 | real pi, dr |
---|
1170 | REAL eps |
---|
1171 | PARAMETER (eps = 1.E-3) |
---|
1172 | !_______________________________________________________________________ |
---|
1173 | |
---|
1174 | ! MU = cosine of solar zenith angle |
---|
1175 | ! RSFC = surface albedo |
---|
1176 | ! TAUU = unscaled optical depth of each layer |
---|
1177 | ! OMU = unscaled single scattering albedo |
---|
1178 | ! GU = unscaled asymmetry factor |
---|
1179 | ! KLEV = max dimension of number of layers in atmosphere |
---|
1180 | ! NLAYER = number of layers in the atmosphere |
---|
1181 | ! NLEVEL = nlayer + 1 = number of levels |
---|
1182 | |
---|
1183 | ! initial conditions: pi*solar flux = 1; diffuse incidence = 0 |
---|
1184 | |
---|
1185 | pifs = 1. |
---|
1186 | fdn0 = 0. |
---|
1187 | |
---|
1188 | nlayer = nlev - 1 |
---|
1189 | |
---|
1190 | pi = acos(-1.) |
---|
1191 | dr = pi/180. |
---|
1192 | mu = COS(zen*dr) |
---|
1193 | |
---|
1194 | !************* compute coefficients for each layer: |
---|
1195 | ! GAM1 - GAM4 = 2-stream coefficients, different for different approximations |
---|
1196 | ! EXPON0 = calculation of e when TAU is zero |
---|
1197 | ! EXPON1 = calculation of e when TAU is TAUN |
---|
1198 | ! CUP and CDN = calculation when TAU is zero |
---|
1199 | ! CUPTN and CDNTN = calc. when TAU is TAUN |
---|
1200 | ! DIVISR = prevents division by zero |
---|
1201 | |
---|
1202 | do j = 0, nlev |
---|
1203 | tauc(j) = 0. |
---|
1204 | tausla(j) = 0. |
---|
1205 | mu2(j) = 1./SQRT(largest) |
---|
1206 | end do |
---|
1207 | |
---|
1208 | IF (.NOT. delta) THEN |
---|
1209 | DO i = 1, nlayer |
---|
1210 | gi(i) = gu(i) |
---|
1211 | omi(i) = omu(i) |
---|
1212 | taun(i) = tauu(i) |
---|
1213 | END DO |
---|
1214 | ELSE |
---|
1215 | |
---|
1216 | ! delta-scaling. Have to be done for delta-Eddington approximation, |
---|
1217 | ! delta discrete ordinate, Practical Improved Flux Method, delta function, |
---|
1218 | ! and Hybrid modified Eddington-delta function methods approximations |
---|
1219 | |
---|
1220 | DO i = 1, nlayer |
---|
1221 | f = gu(i)*gu(i) |
---|
1222 | gi(i) = (gu(i) - f)/(1 - f) |
---|
1223 | omi(i) = (1 - f)*omu(i)/(1 - omu(i)*f) |
---|
1224 | taun(i) = (1 - omu(i)*f)*tauu(i) |
---|
1225 | END DO |
---|
1226 | END IF |
---|
1227 | |
---|
1228 | ! calculate slant optical depth at the top of the atmosphere when zen>90. |
---|
1229 | ! in this case, higher altitude of the top layer is recommended. |
---|
1230 | |
---|
1231 | IF (zen .GT. 90.0) THEN |
---|
1232 | IF (nid(0) .LT. 0) THEN |
---|
1233 | tausla(0) = largest |
---|
1234 | ELSE |
---|
1235 | sum = 0.0 |
---|
1236 | DO j = 1, nid(0) |
---|
1237 | sum = sum + 2.*taun(j)*dsdh(0,j) |
---|
1238 | END DO |
---|
1239 | tausla(0) = sum |
---|
1240 | END IF |
---|
1241 | END IF |
---|
1242 | |
---|
1243 | DO 11, i = 1, nlayer |
---|
1244 | g = gi(i) |
---|
1245 | om = omi(i) |
---|
1246 | tauc(i) = tauc(i-1) + taun(i) |
---|
1247 | |
---|
1248 | ! stay away from 1 by precision. For g, also stay away from -1 |
---|
1249 | |
---|
1250 | tempg = AMIN1(abs(g),1. - precis) |
---|
1251 | g = SIGN(tempg,g) |
---|
1252 | om = AMIN1(om,1.-precis) |
---|
1253 | |
---|
1254 | ! calculate slant optical depth |
---|
1255 | |
---|
1256 | IF (nid(i) .LT. 0) THEN |
---|
1257 | tausla(i) = largest |
---|
1258 | ELSE |
---|
1259 | sum = 0.0 |
---|
1260 | DO j = 1, MIN(nid(i),i) |
---|
1261 | sum = sum + taun(j)*dsdh(i,j) |
---|
1262 | END DO |
---|
1263 | DO j = MIN(nid(i),i)+1,nid(i) |
---|
1264 | sum = sum + 2.*taun(j)*dsdh(i,j) |
---|
1265 | END DO |
---|
1266 | tausla(i) = sum |
---|
1267 | IF (tausla(i) .EQ. tausla(i-1)) THEN |
---|
1268 | mu2(i) = SQRT(largest) |
---|
1269 | ELSE |
---|
1270 | mu2(i) = (tauc(i)-tauc(i-1))/(tausla(i)-tausla(i-1)) |
---|
1271 | mu2(i) = SIGN( AMAX1(ABS(mu2(i)),1./SQRT(largest)), |
---|
1272 | $ mu2(i) ) |
---|
1273 | END IF |
---|
1274 | END IF |
---|
1275 | |
---|
1276 | !** the following gamma equations are from pg 16,289, Table 1 |
---|
1277 | !** save mu1 for each approx. for use in converting irradiance to actinic flux |
---|
1278 | |
---|
1279 | ! Eddington approximation(Joseph et al., 1976, JAS, 33, 2452): |
---|
1280 | |
---|
1281 | c gam1 = (7. - om*(4. + 3.*g))/4. |
---|
1282 | c gam2 = -(1. - om*(4. - 3.*g))/4. |
---|
1283 | c gam3 = (2. - 3.*g*mu)/4. |
---|
1284 | c gam4 = 1. - gam3 |
---|
1285 | c mu1(i) = 0.5 |
---|
1286 | |
---|
1287 | * quadrature (Liou, 1973, JAS, 30, 1303-1326; 1974, JAS, 31, 1473-1475): |
---|
1288 | |
---|
1289 | c gam1 = 1.7320508*(2. - om*(1. + g))/2. |
---|
1290 | c gam2 = 1.7320508*om*(1. - g)/2. |
---|
1291 | c gam3 = (1. - 1.7320508*g*mu)/2. |
---|
1292 | c gam4 = 1. - gam3 |
---|
1293 | c mu1(i) = 1./sqrt(3.) |
---|
1294 | |
---|
1295 | * hemispheric mean (Toon et al., 1089, JGR, 94, 16287): |
---|
1296 | |
---|
1297 | gam1 = 2. - om*(1. + g) |
---|
1298 | gam2 = om*(1. - g) |
---|
1299 | gam3 = (2. - g*mu)/4. |
---|
1300 | gam4 = 1. - gam3 |
---|
1301 | mu1(i) = 0.5 |
---|
1302 | |
---|
1303 | * PIFM (Zdunkovski et al.,1980, Conrib.Atmos.Phys., 53, 147-166): |
---|
1304 | c GAM1 = 0.25*(8. - OM*(5. + 3.*G)) |
---|
1305 | c GAM2 = 0.75*OM*(1.-G) |
---|
1306 | c GAM3 = 0.25*(2.-3.*G*MU) |
---|
1307 | c GAM4 = 1. - GAM3 |
---|
1308 | c mu1(i) = 0.5 |
---|
1309 | |
---|
1310 | * delta discrete ordinates (Schaller, 1979, Contrib.Atmos.Phys, 52, 17-26): |
---|
1311 | c GAM1 = 0.5*1.7320508*(2. - OM*(1. + G)) |
---|
1312 | c GAM2 = 0.5*1.7320508*OM*(1.-G) |
---|
1313 | c GAM3 = 0.5*(1.-1.7320508*G*MU) |
---|
1314 | c GAM4 = 1. - GAM3 |
---|
1315 | c mu1(i) = 1./sqrt(3.) |
---|
1316 | |
---|
1317 | * Calculations of Associated Legendre Polynomials for GAMA1,2,3,4 |
---|
1318 | * in delta-function, modified quadrature, hemispheric constant, |
---|
1319 | * Hybrid modified Eddington-delta function metods, p633,Table1. |
---|
1320 | * W.E.Meador and W.R.Weaver, GAS,1980,v37,p.630 |
---|
1321 | * W.J.Wiscombe and G.W. Grams, GAS,1976,v33,p2440 |
---|
1322 | c YLM0 = 2. |
---|
1323 | c YLM2 = -3.*G*MU |
---|
1324 | c YLM4 = 0.875*G**3*MU*(5.*MU**2-3.) |
---|
1325 | c YLM6=-0.171875*G**5*MU*(15.-70.*MU**2+63.*MU**4) |
---|
1326 | c YLM8=+0.073242*G**7*MU*(-35.+315.*MU**2-693.*MU**4 |
---|
1327 | c *+429.*MU**6) |
---|
1328 | c YLM10=-0.008118*G**9*MU*(315.-4620.*MU**2+18018.*MU**4 |
---|
1329 | c *-25740.*MU**6+12155.*MU**8) |
---|
1330 | c YLM12=0.003685*G**11*MU*(-693.+15015.*MU**2-90090.*MU**4 |
---|
1331 | c *+218790.*MU**6-230945.*MU**8+88179.*MU**10) |
---|
1332 | c YLMS=YLM0+YLM2+YLM4+YLM6+YLM8+YLM10+YLM12 |
---|
1333 | c YLMS=0.25*YLMS |
---|
1334 | c BETA0 = YLMS |
---|
1335 | c |
---|
1336 | c amu1=1./1.7320508 |
---|
1337 | c YLM0 = 2. |
---|
1338 | c YLM2 = -3.*G*amu1 |
---|
1339 | c YLM4 = 0.875*G**3*amu1*(5.*amu1**2-3.) |
---|
1340 | c YLM6=-0.171875*G**5*amu1*(15.-70.*amu1**2+63.*amu1**4) |
---|
1341 | c YLM8=+0.073242*G**7*amu1*(-35.+315.*amu1**2-693.*amu1**4 |
---|
1342 | c *+429.*amu1**6) |
---|
1343 | c YLM10=-0.008118*G**9*amu1*(315.-4620.*amu1**2+18018.*amu1**4 |
---|
1344 | c *-25740.*amu1**6+12155.*amu1**8) |
---|
1345 | c YLM12=0.003685*G**11*amu1*(-693.+15015.*amu1**2-90090.*amu1**4 |
---|
1346 | c *+218790.*amu1**6-230945.*amu1**8+88179.*amu1**10) |
---|
1347 | c YLMS=YLM0+YLM2+YLM4+YLM6+YLM8+YLM10+YLM12 |
---|
1348 | c YLMS=0.25*YLMS |
---|
1349 | c BETA1 = YLMS |
---|
1350 | c |
---|
1351 | c BETAn = 0.25*(2. - 1.5*G-0.21875*G**3-0.085938*G**5 |
---|
1352 | c *-0.045776*G**7) |
---|
1353 | |
---|
1354 | |
---|
1355 | * Hybrid modified Eddington-delta function(Meador and Weaver,1980,JAS,37,630): |
---|
1356 | c subd=4.*(1.-G*G*(1.-MU)) |
---|
1357 | c GAM1 = (7.-3.*G*G-OM*(4.+3.*G)+OM*G*G*(4.*BETA0+3.*G))/subd |
---|
1358 | c GAM2 =-(1.-G*G-OM*(4.-3.*G)-OM*G*G*(4.*BETA0+3.*G-4.))/subd |
---|
1359 | c GAM3 = BETA0 |
---|
1360 | c GAM4 = 1. - GAM3 |
---|
1361 | c mu1(i) = (1. - g*g*(1.- mu) )/(2. - g*g) |
---|
1362 | |
---|
1363 | ***** |
---|
1364 | * delta function (Meador, and Weaver, 1980, JAS, 37, 630): |
---|
1365 | c GAM1 = (1. - OM*(1. - beta0))/MU |
---|
1366 | c GAM2 = OM*BETA0/MU |
---|
1367 | c GAM3 = BETA0 |
---|
1368 | c GAM4 = 1. - GAM3 |
---|
1369 | c mu1(i) = mu |
---|
1370 | ***** |
---|
1371 | * modified quadrature (Meador, and Weaver, 1980, JAS, 37, 630): |
---|
1372 | c GAM1 = 1.7320508*(1. - OM*(1. - beta1)) |
---|
1373 | c GAM2 = 1.7320508*OM*beta1 |
---|
1374 | c GAM3 = BETA0 |
---|
1375 | c GAM4 = 1. - GAM3 |
---|
1376 | c mu1(i) = 1./sqrt(3.) |
---|
1377 | |
---|
1378 | * hemispheric constant (Toon et al., 1989, JGR, 94, 16287): |
---|
1379 | c GAM1 = 2.*(1. - OM*(1. - betan)) |
---|
1380 | c GAM2 = 2.*OM*BETAn |
---|
1381 | c GAM3 = BETA0 |
---|
1382 | c GAM4 = 1. - GAM3 |
---|
1383 | c mu1(i) = 0.5 |
---|
1384 | |
---|
1385 | ***** |
---|
1386 | |
---|
1387 | * lambda = pg 16,290 equation 21 |
---|
1388 | * big gamma = pg 16,290 equation 22 |
---|
1389 | * if gam2 = 0., then bgam = 0. |
---|
1390 | |
---|
1391 | lam(i) = sqrt(gam1*gam1 - gam2*gam2) |
---|
1392 | |
---|
1393 | IF (gam2 .NE. 0.) THEN |
---|
1394 | bgam(i) = (gam1 - lam(i))/gam2 |
---|
1395 | ELSE |
---|
1396 | bgam(i) = 0. |
---|
1397 | END IF |
---|
1398 | |
---|
1399 | expon = EXP(-lam(i)*taun(i)) |
---|
1400 | |
---|
1401 | * e1 - e4 = pg 16,292 equation 44 |
---|
1402 | |
---|
1403 | e1(i) = 1. + bgam(i)*expon |
---|
1404 | e2(i) = 1. - bgam(i)*expon |
---|
1405 | e3(i) = bgam(i) + expon |
---|
1406 | e4(i) = bgam(i) - expon |
---|
1407 | |
---|
1408 | * the following sets up for the C equations 23, and 24 |
---|
1409 | * found on page 16,290 |
---|
1410 | * prevent division by zero (if LAMBDA=1/MU, shift 1/MU^2 by EPS = 1.E-3 |
---|
1411 | * which is approx equiv to shifting MU by 0.5*EPS* (MU)**3 |
---|
1412 | |
---|
1413 | expon0 = EXP(-tausla(i-1)) |
---|
1414 | expon1 = EXP(-tausla(i)) |
---|
1415 | |
---|
1416 | divisr = lam(i)*lam(i) - 1./(mu2(i)*mu2(i)) |
---|
1417 | temp = AMAX1(eps,abs(divisr)) |
---|
1418 | divisr = SIGN(temp,divisr) |
---|
1419 | |
---|
1420 | up = om*pifs*((gam1 - 1./mu2(i))*gam3 + gam4*gam2)/divisr |
---|
1421 | dn = om*pifs*((gam1 + 1./mu2(i))*gam4 + gam2*gam3)/divisr |
---|
1422 | |
---|
1423 | * cup and cdn are when tau is equal to zero |
---|
1424 | * cuptn and cdntn are when tau is equal to taun |
---|
1425 | |
---|
1426 | cup(i) = up*expon0 |
---|
1427 | cdn(i) = dn*expon0 |
---|
1428 | cuptn(i) = up*expon1 |
---|
1429 | cdntn(i) = dn*expon1 |
---|
1430 | |
---|
1431 | 11 CONTINUE |
---|
1432 | |
---|
1433 | ***************** set up matrix ****** |
---|
1434 | * ssfc = pg 16,292 equation 37 where pi Fs is one (unity). |
---|
1435 | |
---|
1436 | ssfc = rsfc*mu*EXP(-tausla(nlayer))*pifs |
---|
1437 | |
---|
1438 | * MROWS = the number of rows in the matrix |
---|
1439 | |
---|
1440 | mrows = 2*nlayer |
---|
1441 | |
---|
1442 | * the following are from pg 16,292 equations 39 - 43. |
---|
1443 | * set up first row of matrix: |
---|
1444 | |
---|
1445 | i = 1 |
---|
1446 | a(1) = 0. |
---|
1447 | b(1) = e1(i) |
---|
1448 | d(1) = -e2(i) |
---|
1449 | e(1) = fdn0 - cdn(i) |
---|
1450 | |
---|
1451 | row=1 |
---|
1452 | |
---|
1453 | * set up odd rows 3 thru (MROWS - 1): |
---|
1454 | |
---|
1455 | i = 0 |
---|
1456 | DO 20, row = 3, mrows - 1, 2 |
---|
1457 | i = i + 1 |
---|
1458 | a(row) = e2(i)*e3(i) - e4(i)*e1(i) |
---|
1459 | b(row) = e1(i)*e1(i + 1) - e3(i)*e3(i + 1) |
---|
1460 | d(row) = e3(i)*e4(i + 1) - e1(i)*e2(i + 1) |
---|
1461 | e(row) = e3(i)*(cup(i + 1) - cuptn(i)) + |
---|
1462 | $ e1(i)*(cdntn(i) - cdn(i + 1)) |
---|
1463 | 20 CONTINUE |
---|
1464 | |
---|
1465 | * set up even rows 2 thru (MROWS - 2): |
---|
1466 | |
---|
1467 | i = 0 |
---|
1468 | DO 30, row = 2, mrows - 2, 2 |
---|
1469 | i = i + 1 |
---|
1470 | a(row) = e2(i + 1)*e1(i) - e3(i)*e4(i + 1) |
---|
1471 | b(row) = e2(i)*e2(i + 1) - e4(i)*e4(i + 1) |
---|
1472 | d(row) = e1(i + 1)*e4(i + 1) - e2(i + 1)*e3(i + 1) |
---|
1473 | e(row) = (cup(i + 1) - cuptn(i))*e2(i + 1) - |
---|
1474 | $ (cdn(i + 1) - cdntn(i))*e4(i + 1) |
---|
1475 | 30 CONTINUE |
---|
1476 | |
---|
1477 | * set up last row of matrix at MROWS: |
---|
1478 | |
---|
1479 | row = mrows |
---|
1480 | i = nlayer |
---|
1481 | |
---|
1482 | a(row) = e1(i) - rsfc*e3(i) |
---|
1483 | b(row) = e2(i) - rsfc*e4(i) |
---|
1484 | d(row) = 0. |
---|
1485 | e(row) = ssfc - cuptn(i) + rsfc*cdntn(i) |
---|
1486 | |
---|
1487 | * solve tri-diagonal matrix: |
---|
1488 | |
---|
1489 | CALL tridiag(a, b, d, e, y, mrows) |
---|
1490 | |
---|
1491 | **** unfold solution of matrix, compute output fluxes: |
---|
1492 | |
---|
1493 | row = 1 |
---|
1494 | lev = 1 |
---|
1495 | j = 1 |
---|
1496 | |
---|
1497 | * the following equations are from pg 16,291 equations 31 & 32 |
---|
1498 | |
---|
1499 | fdr(lev) = EXP( -tausla(0) ) |
---|
1500 | edr(lev) = mu * fdr(lev) |
---|
1501 | edn(lev) = fdn0 |
---|
1502 | eup(lev) = y(row)*e3(j) - y(row + 1)*e4(j) + cup(j) |
---|
1503 | fdn(lev) = edn(lev)/mu1(lev) |
---|
1504 | fup(lev) = eup(lev)/mu1(lev) |
---|
1505 | |
---|
1506 | DO 60, lev = 2, nlayer + 1 |
---|
1507 | fdr(lev) = EXP(-tausla(lev-1)) |
---|
1508 | edr(lev) = mu *fdr(lev) |
---|
1509 | edn(lev) = y(row)*e3(j) + y(row + 1)*e4(j) + cdntn(j) |
---|
1510 | eup(lev) = y(row)*e1(j) + y(row + 1)*e2(j) + cuptn(j) |
---|
1511 | fdn(lev) = edn(lev)/mu1(j) |
---|
1512 | fup(lev) = eup(lev)/mu1(j) |
---|
1513 | |
---|
1514 | row = row + 2 |
---|
1515 | j = j + 1 |
---|
1516 | 60 CONTINUE |
---|
1517 | |
---|
1518 | end subroutine ps2str |
---|
1519 | |
---|
1520 | *=============================================================================* |
---|
1521 | |
---|
1522 | subroutine tridiag(a,b,c,r,u,n) |
---|
1523 | |
---|
1524 | !_______________________________________________________________________ |
---|
1525 | ! solves tridiagonal system. From Numerical Recipies, p. 40 |
---|
1526 | !_______________________________________________________________________ |
---|
1527 | |
---|
1528 | IMPLICIT NONE |
---|
1529 | |
---|
1530 | ! input: |
---|
1531 | |
---|
1532 | INTEGER n |
---|
1533 | REAL a, b, c, r |
---|
1534 | DIMENSION a(n),b(n),c(n),r(n) |
---|
1535 | |
---|
1536 | ! output: |
---|
1537 | |
---|
1538 | REAL u |
---|
1539 | DIMENSION u(n) |
---|
1540 | |
---|
1541 | ! local: |
---|
1542 | |
---|
1543 | INTEGER j |
---|
1544 | |
---|
1545 | REAL bet, gam |
---|
1546 | DIMENSION gam(n) |
---|
1547 | !_______________________________________________________________________ |
---|
1548 | |
---|
1549 | IF (b(1) .EQ. 0.) STOP 1001 |
---|
1550 | bet = b(1) |
---|
1551 | u(1) = r(1)/bet |
---|
1552 | DO 11, j = 2, n |
---|
1553 | gam(j) = c(j - 1)/bet |
---|
1554 | bet = b(j) - a(j)*gam(j) |
---|
1555 | IF (bet .EQ. 0.) STOP 2002 |
---|
1556 | u(j) = (r(j) - a(j)*u(j - 1))/bet |
---|
1557 | 11 CONTINUE |
---|
1558 | DO 12, j = n - 1, 1, -1 |
---|
1559 | u(j) = u(j) - gam(j + 1)*u(j + 1) |
---|
1560 | 12 CONTINUE |
---|
1561 | !_______________________________________________________________________ |
---|
1562 | |
---|
1563 | end subroutine tridiag |
---|
1564 | |
---|
1565 | end subroutine photolysis_online |
---|