1 | ! radiation_lw_derivatives.F90 - Compute longwave derivatives for Hogan and Bozzo (2015) method |
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2 | |
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3 | ! (C) Copyright 2016- ECMWF. |
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4 | |
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5 | ! This software is licensed under the terms of the Apache Licence Version 2.0 |
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6 | ! which can be obtained at http://www.apache.org/licenses/LICENSE-2.0. |
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7 | |
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8 | ! In applying this licence, ECMWF does not waive the privileges and immunities |
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9 | ! granted to it by virtue of its status as an intergovernmental organisation |
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10 | ! nor does it submit to any jurisdiction. |
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11 | |
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12 | ! Author: Robin Hogan |
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13 | ! Email: r.j.hogan@ecmwf.int |
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14 | |
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15 | ! This module provides routines to compute the rate of change of |
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16 | ! broadband upwelling longwave flux at each half level with respect to |
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17 | ! the surface broadband upwelling flux. This is done from the surface |
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18 | ! spectral fluxes and the spectral transmittance of each atmospheric |
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19 | ! layer, assuming no longwave scattering. The result may be used to |
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20 | ! perform approximate updates to the longwave flux profile in between |
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21 | ! calls to the full radiation scheme, accounting for the change in |
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22 | ! skin temperature, following the method of Hogan and Bozzo (JAMES |
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23 | ! 2015). Separate routines are provided for each solver. |
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24 | |
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25 | ! Note that currently a more approximate calculation is performed from |
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26 | ! the exact one in Hogan and Bozzo (2015); here we assume that a |
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27 | ! change in temperature increases the spectral fluxes in proportion, |
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28 | ! when in reality there is a change in shape of the Planck function in |
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29 | ! addition to an overall increase in the total emission. |
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30 | |
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31 | ! Modifications |
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32 | ! 2017-10-23 R. Hogan Renamed single-character variables |
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33 | |
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34 | module radiation_lw_derivatives |
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35 | |
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36 | public |
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37 | |
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38 | contains |
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39 | |
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40 | !--------------------------------------------------------------------- |
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41 | ! Calculation for the Independent Column Approximation |
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42 | subroutine calc_lw_derivatives_ica(ng, nlev, icol, transmittance, flux_up_surf, lw_derivatives) |
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43 | |
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44 | use parkind1, only : jprb |
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45 | use yomhook, only : lhook, dr_hook |
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46 | |
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47 | implicit none |
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48 | |
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49 | ! Inputs |
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50 | integer, intent(in) :: ng ! number of spectral intervals |
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51 | integer, intent(in) :: nlev ! number of levels |
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52 | integer, intent(in) :: icol ! Index of column for output |
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53 | real(jprb), intent(in) :: transmittance(ng,nlev) |
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54 | real(jprb), intent(in) :: flux_up_surf(ng) ! Upwelling surface spectral flux (W m-2) |
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55 | |
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56 | ! Output |
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57 | real(jprb), intent(out) :: lw_derivatives(:,:) ! dimensioned (ncol,nlev+1) |
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58 | |
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59 | ! Rate of change of spectral flux at a given height with respect |
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60 | ! to the surface value |
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61 | real(jprb) :: lw_derivatives_g(ng) |
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62 | |
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63 | integer :: jlev |
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64 | |
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65 | real(jprb) :: hook_handle |
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66 | |
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67 | if (lhook) call dr_hook('radiation_lw_derivatives:calc_lw_derivatives_ica',0,hook_handle) |
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68 | |
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69 | ! Initialize the derivatives at the surface |
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70 | lw_derivatives_g = flux_up_surf / sum(flux_up_surf) |
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71 | lw_derivatives(icol, nlev+1) = 1.0_jprb |
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72 | |
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73 | ! Move up through the atmosphere computing the derivatives at each |
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74 | ! half-level |
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75 | DO jlev = nlev,1,-1 |
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76 | lw_derivatives_g = lw_derivatives_g * transmittance(:,jlev) |
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77 | lw_derivatives(icol,jlev) = sum(lw_derivatives_g) |
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78 | end do |
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79 | |
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80 | if (lhook) call dr_hook('radiation_lw_derivatives:calc_lw_derivatives_ica',1,hook_handle) |
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81 | |
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82 | end subroutine calc_lw_derivatives_ica |
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83 | |
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84 | |
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85 | !--------------------------------------------------------------------- |
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86 | ! Calculation for the Independent Column Approximation |
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87 | subroutine modify_lw_derivatives_ica(ng, nlev, icol, transmittance, & |
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88 | & flux_up_surf, weight, lw_derivatives) |
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89 | |
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90 | use parkind1, only : jprb |
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91 | use yomhook, only : lhook, dr_hook |
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92 | |
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93 | implicit none |
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94 | |
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95 | ! Inputs |
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96 | integer, intent(in) :: ng ! number of spectral intervals |
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97 | integer, intent(in) :: nlev ! number of levels |
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98 | integer, intent(in) :: icol ! Index of column for output |
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99 | real(jprb), intent(in) :: transmittance(ng,nlev) |
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100 | real(jprb), intent(in) :: flux_up_surf(ng) ! Upwelling surface spectral flux (W m-2) |
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101 | real(jprb), intent(in) :: weight ! Weight new values against existing |
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102 | |
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103 | ! Output |
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104 | real(jprb), intent(inout) :: lw_derivatives(:,:) ! dimensioned (ncol,nlev+1) |
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105 | |
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106 | ! Rate of change of spectral flux at a given height with respect |
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107 | ! to the surface value |
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108 | real(jprb) :: lw_derivatives_g(ng) |
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109 | |
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110 | integer :: jlev |
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111 | |
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112 | real(jprb) :: hook_handle |
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113 | |
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114 | if (lhook) call dr_hook('radiation_lw_derivatives:modify_lw_derivatives_ica',0,hook_handle) |
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115 | |
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116 | ! Initialize the derivatives at the surface |
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117 | lw_derivatives_g = flux_up_surf / sum(flux_up_surf) |
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118 | ! This value must be 1 so no weighting applied |
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119 | lw_derivatives(icol, nlev+1) = 1.0_jprb |
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120 | |
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121 | ! Move up through the atmosphere computing the derivatives at each |
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122 | ! half-level |
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123 | DO jlev = nlev,1,-1 |
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124 | lw_derivatives_g = lw_derivatives_g * transmittance(:,jlev) |
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125 | lw_derivatives(icol,jlev) = (1.0_jprb - weight) * lw_derivatives(icol,jlev) & |
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126 | & + weight * sum(lw_derivatives_g) |
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127 | end do |
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128 | |
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129 | if (lhook) call dr_hook('radiation_lw_derivatives:modify_lw_derivatives_ica',1,hook_handle) |
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130 | |
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131 | end subroutine modify_lw_derivatives_ica |
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132 | |
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133 | |
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134 | |
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135 | !--------------------------------------------------------------------- |
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136 | ! Calculation for solvers involving multiple regions and matrices |
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137 | subroutine calc_lw_derivatives_matrix(ng, nlev, nreg, icol, transmittance, & |
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138 | & u_matrix, flux_up_surf, lw_derivatives) |
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139 | |
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140 | use parkind1, only : jprb |
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141 | use yomhook, only : lhook, dr_hook |
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142 | |
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143 | use radiation_matrix |
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144 | |
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145 | implicit none |
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146 | |
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147 | ! Inputs |
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148 | integer, intent(in) :: ng ! number of spectral intervals |
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149 | integer, intent(in) :: nlev ! number of levels |
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150 | integer, intent(in) :: nreg ! number of regions |
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151 | integer, intent(in) :: icol ! Index of column for output |
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152 | real(jprb), intent(in) :: transmittance(ng,nreg,nreg,nlev) |
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153 | real(jprb), intent(in) :: u_matrix(nreg,nreg,nlev+1) ! Upward overlap matrix |
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154 | real(jprb), intent(in) :: flux_up_surf(ng) ! Upwelling surface spectral flux (W m-2) |
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155 | |
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156 | ! Output |
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157 | real(jprb), intent(out) :: lw_derivatives(:,:) ! dimensioned (ncol,nlev+1) |
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158 | |
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159 | ! Rate of change of spectral flux at a given height with respect |
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160 | ! to the surface value |
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161 | real(jprb) :: lw_derivatives_g_reg(ng,nreg) |
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162 | |
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163 | integer :: jlev |
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164 | |
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165 | real(jprb) :: hook_handle |
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166 | |
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167 | if (lhook) call dr_hook('radiation_lw_derivatives:calc_lw_derivatives_matrix',0,hook_handle) |
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168 | |
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169 | ! Initialize the derivatives at the surface; the surface is |
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170 | ! treated as a single clear-sky layer so we only need to put |
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171 | ! values in region 1. |
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172 | lw_derivatives_g_reg = 0.0_jprb |
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173 | lw_derivatives_g_reg(:,1) = flux_up_surf / sum(flux_up_surf) |
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174 | lw_derivatives(icol, nlev+1) = 1.0_jprb |
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175 | |
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176 | ! Move up through the atmosphere computing the derivatives at each |
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177 | ! half-level |
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178 | DO jlev = nlev,1,-1 |
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179 | ! Compute effect of overlap at half-level jlev+1, yielding |
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180 | ! derivatives just above that half-level |
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181 | lw_derivatives_g_reg = singlemat_x_vec(ng,ng,nreg,u_matrix(:,:,jlev+1),lw_derivatives_g_reg) |
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182 | |
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183 | ! Compute effect of transmittance of layer jlev, yielding |
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184 | ! derivatives just below the half-level above (jlev) |
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185 | lw_derivatives_g_reg = mat_x_vec(ng,ng,nreg,transmittance(:,:,:,jlev),lw_derivatives_g_reg) |
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186 | |
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187 | lw_derivatives(icol, jlev) = sum(lw_derivatives_g_reg) |
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188 | end do |
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189 | |
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190 | if (lhook) call dr_hook('radiation_lw_derivatives:calc_lw_derivatives_matrix',1,hook_handle) |
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191 | |
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192 | end subroutine calc_lw_derivatives_matrix |
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193 | |
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194 | |
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195 | !--------------------------------------------------------------------- |
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196 | ! Calculation for solvers involving multiple regions but no 3D |
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197 | ! effects: the difference from calc_lw_derivatives_matrix is that transmittance |
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198 | ! has one less dimensions |
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199 | subroutine calc_lw_derivatives_region(ng, nlev, nreg, icol, transmittance, & |
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200 | & u_matrix, flux_up_surf, lw_derivatives) |
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201 | |
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202 | use parkind1, only : jprb |
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203 | use yomhook, only : lhook, dr_hook |
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204 | |
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205 | use radiation_matrix |
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206 | |
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207 | implicit none |
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208 | |
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209 | ! Inputs |
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210 | integer, intent(in) :: ng ! number of spectral intervals |
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211 | integer, intent(in) :: nlev ! number of levels |
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212 | integer, intent(in) :: nreg ! number of regions |
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213 | integer, intent(in) :: icol ! Index of column for output |
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214 | real(jprb), intent(in) :: transmittance(ng,nreg,nlev) |
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215 | real(jprb), intent(in) :: u_matrix(nreg,nreg,nlev+1) ! Upward overlap matrix |
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216 | real(jprb), intent(in) :: flux_up_surf(ng) ! Upwelling surface spectral flux (W m-2) |
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217 | |
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218 | ! Output |
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219 | real(jprb), intent(out) :: lw_derivatives(:,:) ! dimensioned (ncol,nlev+1) |
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220 | |
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221 | ! Rate of change of spectral flux at a given height with respect |
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222 | ! to the surface value |
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223 | real(jprb) :: lw_derivatives_g_reg(ng,nreg) |
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224 | |
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225 | integer :: jlev |
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226 | |
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227 | real(jprb) :: hook_handle |
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228 | |
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229 | if (lhook) call dr_hook('radiation_lw_derivatives:calc_lw_derivatives_region',0,hook_handle) |
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230 | |
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231 | ! Initialize the derivatives at the surface; the surface is |
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232 | ! treated as a single clear-sky layer so we only need to put |
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233 | ! values in region 1. |
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234 | lw_derivatives_g_reg = 0.0_jprb |
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235 | lw_derivatives_g_reg(:,1) = flux_up_surf / sum(flux_up_surf) |
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236 | lw_derivatives(icol, nlev+1) = 1.0_jprb |
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237 | |
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238 | ! Move up through the atmosphere computing the derivatives at each |
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239 | ! half-level |
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240 | DO jlev = nlev,1,-1 |
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241 | ! Compute effect of overlap at half-level jlev+1, yielding |
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242 | ! derivatives just above that half-level |
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243 | lw_derivatives_g_reg = singlemat_x_vec(ng,ng,nreg,u_matrix(:,:,jlev+1),lw_derivatives_g_reg) |
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244 | |
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245 | ! Compute effect of transmittance of layer jlev, yielding |
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246 | ! derivatives just below the half-level above (jlev) |
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247 | lw_derivatives_g_reg = transmittance(:,:,jlev) * lw_derivatives_g_reg |
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248 | |
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249 | lw_derivatives(icol, jlev) = sum(lw_derivatives_g_reg) |
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250 | end do |
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251 | |
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252 | if (lhook) call dr_hook('radiation_lw_derivatives:calc_lw_derivatives_region',1,hook_handle) |
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253 | |
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254 | end subroutine calc_lw_derivatives_region |
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255 | |
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256 | |
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257 | end module radiation_lw_derivatives |
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