1 | SUBROUTINE SFLUXV(DTAUV,TAUV,TAUCUMV,RSFV,DWNV,WBARV,COSBV, |
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2 | * UBAR0,STEL,GWEIGHT,NFLUXTOPV,FLUXTOPVDN, |
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3 | * NFLUXOUTV_nu,NFLUXGNDV_nu, |
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4 | * FMNETV,FLUXUPV,FLUXDNV,FZEROV,taugsurf) |
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5 | |
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6 | use radinc_h |
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7 | use radcommon_h, only: tlimit |
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8 | |
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9 | implicit none |
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10 | |
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11 | real*8 FMNETV(L_NLAYRAD) |
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12 | real*8 TAUCUMV(L_LEVELS,L_NSPECTV,L_NGAUSS) |
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13 | real*8 TAUV(L_NLEVRAD,L_NSPECTV,L_NGAUSS) |
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14 | real*8 DTAUV(L_NLAYRAD,L_NSPECTV,L_NGAUSS), DWNV(L_NSPECTV) |
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15 | real*8 FMUPV(L_NLAYRAD), FMDV(L_NLAYRAD) |
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16 | real*8 COSBV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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17 | real*8 WBARV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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18 | real*8 STEL(L_NSPECTV) |
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19 | real*8 FLUXUPV(L_NLAYRAD), FLUXDNV(L_NLAYRAD) |
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20 | real*8 NFLUXTOPV, FLUXUP, FLUXDN,FLUXTOPVDN |
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21 | real*8 NFLUXOUTV_nu(L_NSPECTV) |
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22 | real*8 NFLUXGNDV_nu(L_NSPECTV) |
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23 | real*8 GWEIGHT(L_NGAUSS) |
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24 | |
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25 | integer L, NG, NW, NG1,k |
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26 | real*8 rsfv, ubar0, f0pi, btop, bsurf, taumax, eterm |
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27 | real*8 FZEROV(L_NSPECTV) |
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28 | |
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29 | real*8 DIFFV, DIFFVT |
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30 | real*8 taugsurf(L_NSPECTV,L_NGAUSS-1), fzero |
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31 | |
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32 | C======================================================================C |
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33 | |
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34 | TAUMAX = L_TAUMAX |
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35 | |
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36 | C ZERO THE NET FLUXES |
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37 | |
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38 | NFLUXTOPV = 0.0 |
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39 | FLUXTOPVDN = 0.0 |
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40 | |
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41 | DO NW=1,L_NSPECTV |
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42 | NFLUXOUTV_nu(NW)=0.0 |
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43 | NFLUXGNDV_nu(NW)=0.0 |
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44 | END DO |
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45 | |
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46 | DO L=1,L_NLAYRAD |
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47 | FMNETV(L) = 0.0 |
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48 | FLUXUPV(L) = 0.0 |
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49 | FLUXDNV(L) = 0.0 |
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50 | END DO |
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51 | |
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52 | DIFFVT = 0.0 |
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53 | |
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54 | C WE NOW ENTER A MAJOR LOOP OVER SPECTRAL INTERVALS IN THE VISIBLE |
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55 | C TO CALCULATE THE NET FLUX IN EACH SPECTRAL INTERVAL |
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56 | |
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57 | DO 500 NW=1,L_NSPECTV |
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58 | |
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59 | F0PI = STEL(NW) |
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60 | |
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61 | FZERO = FZEROV(NW) |
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62 | IF(FZERO.ge.0.99) goto 40 |
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63 | DO NG=1,L_NGAUSS-1 |
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64 | |
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65 | if(TAUGSURF(NW,NG) .lt. TLIMIT) then |
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66 | |
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67 | fzero = fzero + (1.0-FZEROV(NW))*GWEIGHT(NG) |
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68 | |
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69 | goto 30 |
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70 | end if |
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71 | |
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72 | C SET UP THE UPPER AND LOWER BOUNDARY CONDITIONS ON THE VISIBLE |
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73 | |
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74 | BTOP = 0.0 |
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75 | !BSURF = 0./0. ! why was this here? |
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76 | BSURF = 0. |
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77 | C LOOP OVER THE NTERMS BEGINNING HERE |
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78 | |
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79 | |
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80 | ! FACTOR = 1.0D0 - WDEL(1)*CDEL(1)**2 |
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81 | ! TAU(1) = TDEL(1)*FACTOR |
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82 | |
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83 | |
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84 | ETERM = MIN(TAUV(L_NLEVRAD,NW,NG),TAUMAX) |
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85 | BSURF = RSFV*UBAR0*STEL(NW)*EXP(-ETERM/UBAR0) |
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86 | |
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87 | C WE CAN NOW SOLVE FOR THE COEFFICIENTS OF THE TWO STREAM |
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88 | C CALL A SUBROUTINE THAT SOLVES FOR THE FLUX TERMS |
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89 | C WITHIN EACH INTERVAL AT THE MIDPOINT WAVENUMBER |
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90 | C |
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91 | C FUW AND FDW ARE WORKING FLUX ARRAYS THAT WILL BE USED TO |
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92 | C RETURN FLUXES FOR A GIVEN NT |
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93 | |
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94 | |
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95 | CALL GFLUXV(DTAUV(1,NW,NG),TAUV(1,NW,NG),TAUCUMV(1,NW,NG), |
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96 | * WBARV(1,NW,NG),COSBV(1,NW,NG),UBAR0,F0PI,RSFV, |
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97 | * BTOP,BSURF,FMUPV,FMDV,DIFFV,FLUXUP,FLUXDN) |
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98 | |
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99 | C NOW CALCULATE THE CUMULATIVE VISIBLE NET FLUX |
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100 | |
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101 | NFLUXTOPV = NFLUXTOPV+(FLUXUP-FLUXDN)*GWEIGHT(NG)* |
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102 | * (1.0-FZEROV(NW)) |
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103 | FLUXTOPVDN = FLUXTOPVDN+FLUXDN*GWEIGHT(NG)* |
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104 | * (1.0-FZEROV(NW)) |
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105 | DO L=1,L_NLAYRAD |
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106 | FMNETV(L)=FMNETV(L)+( FMUPV(L)-FMDV(L) )* |
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107 | * GWEIGHT(NG)*(1.0-FZEROV(NW)) |
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108 | FLUXUPV(L) = FLUXUPV(L) + FMUPV(L)*GWEIGHT(NG)* |
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109 | * (1.0-FZEROV(NW)) |
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110 | FLUXDNV(L) = FLUXDNV(L) + FMDV(L)*GWEIGHT(NG)* |
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111 | * (1.0-FZEROV(NW)) |
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112 | END DO |
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113 | |
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114 | c band-resolved flux leaving TOA (RDW) |
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115 | NFLUXOUTV_nu(NW) = NFLUXOUTV_nu(NW) |
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116 | * +FLUXUP*GWEIGHT(NG)*(1.0-FZEROV(NW)) |
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117 | |
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118 | c band-resolved flux at ground (RDW) |
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119 | NFLUXGNDV_nu(NW) = NFLUXGNDV_nu(NW) |
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120 | * +FMDV(L_NLAYRAD)*GWEIGHT(NG)*(1.0-FZEROV(NW)) |
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121 | |
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122 | |
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123 | C THE DIFFUSE COMPONENT OF THE DOWNWARD STELLAR FLUX |
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124 | |
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125 | DIFFVT = DIFFVT + DIFFV*GWEIGHT(NG)*(1.0-FZEROV(NW)) |
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126 | |
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127 | 30 CONTINUE |
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128 | |
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129 | END DO ! the Gauss loop |
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130 | |
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131 | 40 continue |
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132 | C Special 17th Gauss point |
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133 | |
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134 | NG = L_NGAUSS |
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135 | |
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136 | C SET UP THE UPPER AND LOWER BOUNDARY CONDITIONS ON THE VISIBLE |
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137 | |
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138 | BTOP = 0.0 |
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139 | |
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140 | C LOOP OVER THE NTERMS BEGINNING HERE |
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141 | |
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142 | ETERM = MIN(TAUV(L_NLEVRAD,NW,NG),TAUMAX) |
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143 | BSURF = RSFV*UBAR0*STEL(NW)*EXP(-ETERM/UBAR0) |
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144 | |
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145 | |
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146 | C WE CAN NOW SOLVE FOR THE COEFFICIENTS OF THE TWO STREAM |
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147 | C CALL A SUBROUTINE THAT SOLVES FOR THE FLUX TERMS |
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148 | C WITHIN EACH INTERVAL AT THE MIDPOINT WAVENUMBER |
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149 | C |
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150 | C FUW AND FDW ARE WORKING FLUX ARRAYS THAT WILL BE USED TO |
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151 | C RETURN FLUXES FOR A GIVEN NT |
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152 | |
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153 | CALL GFLUXV(DTAUV(1,NW,NG),TAUV(1,NW,NG),TAUCUMV(1,NW,NG), |
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154 | * WBARV(1,NW,NG),COSBV(1,NW,NG),UBAR0,F0PI,RSFV, |
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155 | * BTOP,BSURF,FMUPV,FMDV,DIFFV,FLUXUP,FLUXDN) |
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156 | |
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157 | |
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158 | C NOW CALCULATE THE CUMULATIVE VISIBLE NET FLUX |
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159 | |
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160 | NFLUXTOPV = NFLUXTOPV+(FLUXUP-FLUXDN)*FZERO |
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161 | FLUXTOPVDN = FLUXTOPVDN+FLUXDN*FZERO |
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162 | DO L=1,L_NLAYRAD |
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163 | FMNETV(L)=FMNETV(L)+( FMUPV(L)-FMDV(L) )*FZERO |
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164 | FLUXUPV(L) = FLUXUPV(L) + FMUPV(L)*FZERO |
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165 | FLUXDNV(L) = FLUXDNV(L) + FMDV(L)*FZERO |
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166 | END DO |
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167 | |
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168 | c band-resolved flux leaving TOA (RDW) |
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169 | NFLUXOUTV_nu(NW) = NFLUXOUTV_nu(NW) |
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170 | * +FLUXUP*FZERO |
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171 | |
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172 | c band-resolved flux at ground (RDW) |
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173 | NFLUXGNDV_nu(NW) = NFLUXGNDV_nu(NW)+FMDV(L_NLAYRAD)*FZERO |
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174 | |
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175 | |
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176 | C THE DIFFUSE COMPONENT OF THE DOWNWARD STELLAR FLUX |
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177 | |
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178 | DIFFVT = DIFFVT + DIFFV*FZERO |
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179 | |
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180 | |
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181 | 500 CONTINUE |
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182 | |
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183 | |
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184 | C *** END OF MAJOR SPECTRAL INTERVAL LOOP IN THE VISIBLE***** |
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185 | |
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186 | |
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187 | RETURN |
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188 | END |
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