1 | SUBROUTINE SFLUXI(PLEV,TLEV,DTAUI,TAUCUMI,UBARI,RSFI,WNOI,DWNI, |
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2 | * COSBI,WBARI,GWEIGHT,NFLUXTOPI,NFLUXTOPI_nu, |
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3 | * FMNETI,fluxupi,fluxdni,fluxupi_nu, |
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4 | * FZEROI,TAUGSURF) |
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5 | |
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6 | use radinc_h |
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7 | use radcommon_h, only: planckir, tlimit |
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8 | |
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9 | implicit none |
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10 | |
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11 | #include "comcstfi.h" |
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12 | |
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13 | integer NLEVRAD, L, NW, NG, NTS, NTT |
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14 | |
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15 | real*8 TLEV(L_LEVELS), PLEV(L_LEVELS) |
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16 | real*8 TAUCUMI(L_LEVELS,L_NSPECTI,L_NGAUSS) |
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17 | real*8 FMNETI(L_NLAYRAD) |
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18 | real*8 WNOI(L_NSPECTI), DWNI(L_NSPECTI) |
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19 | real*8 DTAUI(L_NLAYRAD,L_NSPECTI,L_NGAUSS) |
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20 | real*8 FMUPI(L_NLEVRAD), FMDI(L_NLEVRAD) |
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21 | real*8 COSBI(L_NLAYRAD,L_NSPECTI,L_NGAUSS) |
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22 | real*8 WBARI(L_NLAYRAD,L_NSPECTI,L_NGAUSS) |
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23 | real*8 GWEIGHT(L_NGAUSS), NFLUXTOPI |
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24 | real*8 NFLUXTOPI_nu(L_NSPECTI) |
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25 | real*8 fluxupi_nu(L_NLAYRAD,L_NSPECTI) |
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26 | real*8 FTOPUP |
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27 | |
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28 | real*8 UBARI, RSFI, TSURF, BSURF, TTOP, BTOP, TAUTOP |
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29 | real*8 PLANCK, PLTOP |
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30 | real*8 fluxupi(L_NLAYRAD), fluxdni(L_NLAYRAD) |
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31 | real*8 FZEROI(L_NSPECTI) |
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32 | real*8 taugsurf(L_NSPECTI,L_NGAUSS-1), fzero |
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33 | |
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34 | real*8 fup_tmp(L_NSPECTI),fdn_tmp(L_NSPECTI) |
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35 | |
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36 | |
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37 | C======================================================================C |
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38 | |
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39 | NLEVRAD = L_NLEVRAD |
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40 | |
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41 | |
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42 | C ZERO THE NET FLUXES |
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43 | |
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44 | NFLUXTOPI = 0.0 |
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45 | |
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46 | DO NW=1,L_NSPECTI |
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47 | NFLUXTOPI_nu(NW) = 0.0 |
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48 | DO L=1,L_NLAYRAD |
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49 | FLUXUPI_nu(L,NW) = 0.0 |
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50 | |
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51 | fup_tmp(nw)=0.0 |
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52 | fdn_tmp(nw)=0.0 |
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53 | |
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54 | END DO |
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55 | END DO |
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56 | |
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57 | DO L=1,L_NLAYRAD |
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58 | FMNETI(L) = 0.0 |
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59 | FLUXUPI(L) = 0.0 |
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60 | FLUXDNI(L) = 0.0 |
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61 | END DO |
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62 | |
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63 | C WE NOW ENTER A MAJOR LOOP OVER SPECTRAL INTERVALS IN THE INFRARED |
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64 | C TO CALCULATE THE NET FLUX IN EACH SPECTRAL INTERVAL |
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65 | |
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66 | TTOP = TLEV(2) |
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67 | TSURF = TLEV(L_LEVELS) |
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68 | |
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69 | NTS = int(TSURF*10.0D0)-NTstar+1 |
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70 | NTT = int(TTOP *10.0D0)-NTstar+1 |
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71 | ! NTS = TSURF*10.0D0-499 |
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72 | ! NTT = TTOP *10.0D0-499 |
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73 | |
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74 | DO 501 NW=1,L_NSPECTI |
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75 | |
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76 | C SURFACE EMISSIONS - INDEPENDENT OF GAUSS POINTS |
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77 | BSURF = (1.-RSFI)*PLANCKIR(NW,NTS) ! interpolate for accuracy?? |
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78 | PLTOP = PLANCKIR(NW,NTT) |
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79 | |
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80 | C If FZEROI(NW) = 1, then the k-coefficients are zero - skip to the |
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81 | C special Gauss point at the end. |
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82 | |
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83 | FZERO = FZEROI(NW) |
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84 | IF(FZERO.ge.0.99) goto 40 |
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85 | |
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86 | DO NG=1,L_NGAUSS-1 |
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87 | |
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88 | if(TAUGSURF(NW,NG).lt. TLIMIT) then |
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89 | fzero = fzero + (1.0-FZEROI(NW))*GWEIGHT(NG) |
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90 | goto 30 |
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91 | end if |
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92 | |
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93 | C SET UP THE UPPER AND LOWER BOUNDARY CONDITIONS ON THE IR |
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94 | C CALCULATE THE DOWNWELLING RADIATION AT THE TOP OF THE MODEL |
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95 | C OR THE TOP LAYER WILL COOL TO SPACE UNPHYSICALLY |
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96 | |
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97 | TAUTOP = DTAUI(1,NW,NG)*PLEV(2)/(PLEV(4)-PLEV(2)) |
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98 | BTOP = (1.0-EXP(-TAUTOP/UBARI))*PLTOP |
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99 | |
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100 | C WE CAN NOW SOLVE FOR THE COEFFICIENTS OF THE TWO STREAM |
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101 | C CALL A SUBROUTINE THAT SOLVES FOR THE FLUX TERMS |
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102 | C WITHIN EACH INTERVAL AT THE MIDPOINT WAVENUMBER |
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103 | |
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104 | CALL GFLUXI(NLEVRAD,TLEV,NW,DWNI(NW),DTAUI(1,NW,NG), |
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105 | * TAUCUMI(1,NW,NG), |
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106 | * WBARI(1,NW,NG),COSBI(1,NW,NG),UBARI,RSFI,BTOP, |
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107 | * BSURF,FTOPUP,FMUPI,FMDI) |
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108 | |
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109 | |
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110 | |
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111 | C NOW CALCULATE THE CUMULATIVE IR NET FLUX |
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112 | |
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113 | NFLUXTOPI = NFLUXTOPI+FTOPUP*DWNI(NW)*GWEIGHT(NG)* |
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114 | * (1.0-FZEROI(NW)) |
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115 | |
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116 | c and same thing by spectral band... (RDW) |
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117 | NFLUXTOPI_nu(NW) = NFLUXTOPI_nu(NW) |
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118 | * +FTOPUP*DWNI(NW)*GWEIGHT(NG)*(1.0-FZEROI(NW)) |
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119 | |
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120 | |
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121 | DO L=1,L_NLEVRAD-1 |
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122 | |
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123 | C CORRECT FOR THE WAVENUMBER INTERVALS |
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124 | |
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125 | FMNETI(L) = FMNETI(L)+(FMUPI(L)-FMDI(L))*DWNI(NW)* |
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126 | * GWEIGHT(NG)*(1.0-FZEROI(NW)) |
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127 | FLUXUPI(L) = FLUXUPI(L) + FMUPI(L)*DWNI(NW)*GWEIGHT(NG)* |
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128 | * (1.0-FZEROI(NW)) |
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129 | FLUXDNI(L) = FLUXDNI(L) + FMDI(L)*DWNI(NW)*GWEIGHT(NG)* |
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130 | * (1.0-FZEROI(NW)) |
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131 | |
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132 | c and same thing by spectral band... (RW) |
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133 | FLUXUPI_nu(L,NW) = FLUXUPI_nu(L,NW) + |
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134 | * FMUPI(L)*DWNI(NW)*GWEIGHT(NG)*(1.0-FZEROI(NW)) |
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135 | |
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136 | END DO |
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137 | |
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138 | 30 CONTINUE |
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139 | |
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140 | END DO !End NGAUSS LOOP |
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141 | |
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142 | 40 CONTINUE |
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143 | |
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144 | C SPECIAL 17th Gauss point |
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145 | |
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146 | NG = L_NGAUSS |
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147 | |
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148 | TAUTOP = DTAUI(1,NW,NG)*PLEV(2)/(PLEV(4)-PLEV(2)) |
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149 | BTOP = (1.0-EXP(-TAUTOP/UBARI))*PLTOP |
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150 | |
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151 | C WE CAN NOW SOLVE FOR THE COEFFICIENTS OF THE TWO STREAM |
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152 | C CALL A SUBROUTINE THAT SOLVES FOR THE FLUX TERMS |
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153 | C WITHIN EACH INTERVAL AT THE MIDPOINT WAVENUMBER |
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154 | |
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155 | |
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156 | CALL GFLUXI(NLEVRAD,TLEV,NW,DWNI(NW),DTAUI(1,NW,NG), |
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157 | * TAUCUMI(1,NW,NG), |
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158 | * WBARI(1,NW,NG),COSBI(1,NW,NG),UBARI,RSFI,BTOP, |
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159 | * BSURF,FTOPUP,FMUPI,FMDI) |
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160 | |
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161 | C NOW CALCULATE THE CUMULATIVE IR NET FLUX |
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162 | |
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163 | NFLUXTOPI = NFLUXTOPI+FTOPUP*DWNI(NW)*FZERO |
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164 | |
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165 | c and same thing by spectral band... (RW) |
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166 | NFLUXTOPI_nu(NW) = NFLUXTOPI_nu(NW) |
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167 | * +FTOPUP*DWNI(NW)*FZERO |
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168 | |
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169 | DO L=1,L_NLEVRAD-1 |
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170 | |
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171 | C CORRECT FOR THE WAVENUMBER INTERVALS |
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172 | |
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173 | FMNETI(L) = FMNETI(L)+(FMUPI(L)-FMDI(L))*DWNI(NW)*FZERO |
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174 | FLUXUPI(L) = FLUXUPI(L) + FMUPI(L)*DWNI(NW)*FZERO |
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175 | FLUXDNI(L) = FLUXDNI(L) + FMDI(L)*DWNI(NW)*FZERO |
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176 | |
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177 | c and same thing by spectral band... (RW) |
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178 | FLUXUPI_nu(L,NW) = FLUXUPI_nu(L,NW) + FMUPI(L)*DWNI(NW)*FZERO |
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179 | |
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180 | END DO |
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181 | |
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182 | 501 CONTINUE !End Spectral Interval LOOP |
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183 | |
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184 | C *** END OF MAJOR SPECTRAL INTERVAL LOOP IN THE INFRARED**** |
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185 | |
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186 | RETURN |
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187 | END |
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