| [38] | 1 | subroutine lwflux (ig0,kdlon,kflev,dp |
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| 2 | . ,bsurf,btop,blev,blay,dbsublay |
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| 3 | . ,tlay, tlev, dt0 ! pour sortie dans g2d uniquement |
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| 4 | . ,emis |
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| 5 | . , tautotal,omegtotal,gtotal |
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| 6 | . ,coolrate,fluxground,fluxtop |
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| 7 | . ,netrad) |
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| 8 | |
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| 9 | c---------------------------------------------------------------------- |
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| 10 | c LWFLUX computes the fluxes |
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| 11 | c---------------------------------------------------------------------- |
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| 12 | |
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| [1047] | 13 | use dimradmars_mod, only: ndlo2, nir, ndlon, nuco2, nflev |
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| 14 | use yomlw_h, only: nlaylte, xi, xi_ground, gcp |
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| [38] | 15 | implicit none |
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| 16 | |
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| [1917] | 17 | include "callkeys.h" |
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| 18 | include "comg1d.h" |
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| [38] | 19 | |
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| 20 | c---------------------------------------------------------------------- |
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| 21 | c 0.1 arguments |
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| 22 | c --------- |
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| 23 | c inputs: |
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| 24 | c ------- |
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| [1917] | 25 | integer,intent(in) :: ig0 |
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| 26 | integer,intent(in) :: kdlon ! part of ngrid |
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| 27 | integer,intent(in) :: kflev ! part of nlayer |
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| [38] | 28 | |
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| [1917] | 29 | real,intent(in) :: dp (ndlo2,kflev) ! layer pressure thickness (Pa) |
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| [38] | 30 | |
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| [1917] | 31 | real,intent(in) :: bsurf (ndlo2,nir) ! surface spectral planck function |
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| 32 | real,intent(in) :: blev (ndlo2,nir,kflev+1) ! level spectral planck function |
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| 33 | real,intent(in) :: blay (ndlo2,nir,kflev) ! layer spectral planck function |
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| 34 | real,intent(in) :: btop (ndlo2,nir) ! top spectral planck function |
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| 35 | real,intent(in) :: dbsublay (ndlo2,nir,2*kflev) ! layer gradient spectral planck |
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| 36 | ! function in sub layers |
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| [38] | 37 | |
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| [1917] | 38 | real,intent(in) :: dt0 (ndlo2) ! surface temperature discontinuity |
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| 39 | real,intent(in) :: tlay (ndlo2,kflev) ! layer temperature |
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| 40 | real,intent(in) :: tlev (ndlo2,kflev+1) ! level temperature |
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| [38] | 41 | |
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| [1917] | 42 | real,intent(in) :: emis (ndlo2) ! surface emissivity |
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| [38] | 43 | |
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| [1917] | 44 | real,intent(in) :: tautotal(ndlo2,kflev,nir) ! \ Total single scattering |
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| 45 | real,intent(in) :: omegtotal(ndlo2,kflev,nir) ! > properties (Addition of the |
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| 46 | real,intent(in) :: gtotal(ndlo2,kflev,nir) ! / NAERKIND aerosols prop.) |
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| [38] | 47 | |
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| 48 | |
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| 49 | c outputs: |
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| 50 | c -------- |
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| [1917] | 51 | real,intent(out) :: coolrate(ndlo2,kflev) ! radiative cooling rate (K/s) |
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| 52 | real,intent(out) :: netrad (ndlo2,kflev) ! radiative budget (W/m2) |
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| 53 | real,intent(out) :: fluxground(ndlo2) ! downward flux on the ground |
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| 54 | ! for surface radiative budget |
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| 55 | real,intent(out) :: fluxtop(ndlo2) ! upward flux on the top of atm ("OLR") |
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| [38] | 56 | |
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| 57 | |
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| 58 | c---------------------------------------------------------------------- |
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| 59 | c 0.2 local arrays |
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| 60 | c ------------ |
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| 61 | |
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| [1917] | 62 | integer ja,jl,j,i,ig1d,ig,l |
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| [38] | 63 | real ksidb (ndlon,nuco2+1,0:nflev+1,0:nflev+1) ! net exchange rate (W/m2) |
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| 64 | |
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| 65 | real dpsgcp (0:nflev+1,0:nflev+1) ! dp/(g.cp) |
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| 66 | real temp (0:nflev+1,0:nflev+1) |
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| 67 | |
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| 68 | real fluxdiff(ndlon,2,nflev+1) ! diffusion flux: upward(1) downward(2) |
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| 69 | |
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| 70 | real*4 reel4 |
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| 71 | |
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| 72 | c To compute IR flux in the atmosphere (For diagnostic only !!) |
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| 73 | logical computeflux |
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| [1047] | 74 | real coefd(kdlon,nuco2,nflev+1,nflev+1) |
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| 75 | real coefu(kdlon,nuco2,0:nflev,nflev+1) |
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| 76 | real flw_up(kdlon,nflev+1), flw_dn(kdlon,nflev+1) ! fluxes (W/m2) |
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| [38] | 77 | |
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| 78 | |
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| [1917] | 79 | ksidb(:,:,:,:)=0 |
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| [38] | 80 | |
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| 81 | c---------------------------------------------------------------------- |
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| 82 | c 1.1 exchanges (layer i <--> all layers up to i) |
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| 83 | c ------------------------------------------- |
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| 84 | |
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| 85 | do i = 1,nlaylte |
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| 86 | do j = i+1,nlaylte |
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| 87 | do ja = 1,nuco2 |
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| 88 | do jl = 1,kdlon |
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| 89 | |
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| 90 | ksidb(jl,ja,i,j) = xi(ig0+jl,ja,i,j) |
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| 91 | . * (blay(jl,ja,j)-blay(jl,ja,i)) |
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| 92 | c ksidb reciprocity |
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| 93 | c ----------------- |
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| 94 | ksidb(jl,ja,j,i) = -ksidb(jl,ja,i,j) |
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| 95 | |
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| 96 | enddo |
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| 97 | enddo |
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| 98 | enddo |
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| 99 | enddo |
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| 100 | |
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| 101 | c---------------------------------------------------------------------- |
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| 102 | c 1.2 exchanges (ground <--> all layers) |
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| 103 | c ---------------------------------- |
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| 104 | |
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| 105 | do i = 1,nlaylte |
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| 106 | do ja = 1,nuco2 |
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| 107 | do jl = 1,kdlon |
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| 108 | |
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| 109 | ksidb(jl,ja,i,0) = xi(ig0+jl,ja,0,i) |
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| 110 | . * (bsurf(jl,ja)-blay(jl,ja,i)) |
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| 111 | c ksidb reciprocity |
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| 112 | c ----------------- |
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| 113 | ksidb(jl,ja,0,i) = -ksidb(jl,ja,i,0) |
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| 114 | |
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| 115 | enddo |
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| 116 | enddo |
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| 117 | enddo |
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| 118 | |
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| 119 | c-------------------------------------------------------- |
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| 120 | c Here we add the neighbour contribution |
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| 121 | c for exchanges between ground and first layer |
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| 122 | c-------------------------------------------------------- |
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| 123 | |
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| 124 | do ja = 1,nuco2 |
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| 125 | do jl = 1,kdlon |
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| 126 | |
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| 127 | ksidb(jl,ja,1,0) = ksidb(jl,ja,1,0) |
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| 128 | . - xi_ground(ig0+jl,ja) |
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| 129 | . * (blev(jl,ja,1)-blay(jl,ja,1)) |
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| 130 | |
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| 131 | cc ksidb reciprocity |
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| 132 | cc ----------------- |
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| 133 | ksidb(jl,ja,0,1) = - ksidb(jl,ja,1,0) |
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| 134 | |
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| 135 | enddo |
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| 136 | enddo |
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| 137 | |
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| 138 | c---------------------------------------------------------------------- |
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| 139 | c 1.3 exchanges (layer i <--> space) |
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| 140 | c ------------------------------ |
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| 141 | |
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| 142 | do i = 1,nlaylte |
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| 143 | do ja = 1,nuco2 |
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| 144 | do jl = 1,kdlon |
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| 145 | |
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| 146 | ksidb(jl,ja,i,nlaylte+1) = xi(ig0+jl,ja,i,nlaylte+1) |
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| 147 | . * (-blay(jl,ja,i)) |
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| 148 | c ksidb reciprocity |
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| 149 | c ----------------- |
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| 150 | ksidb(jl,ja,nlaylte+1,i) = - ksidb(jl,ja,i,nlaylte+1) |
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| 151 | |
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| 152 | enddo |
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| 153 | enddo |
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| 154 | enddo |
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| 155 | |
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| 156 | c---------------------------------------------------------------------- |
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| 157 | c 1.4 exchanges (ground <--> space) |
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| 158 | c ----------------------------- |
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| 159 | |
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| 160 | do ja = 1,nuco2 |
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| 161 | do jl = 1,kdlon |
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| 162 | |
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| 163 | ksidb(jl,ja,0,nlaylte+1) = xi(ig0+jl,ja,0,nlaylte+1) |
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| 164 | . * (-bsurf(jl,ja)) |
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| 165 | |
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| 166 | c ksidb reciprocity |
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| 167 | c ----------------- |
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| 168 | ksidb(jl,ja,nlaylte+1,0) = - ksidb(jl,ja,0,nlaylte+1) |
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| 169 | |
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| 170 | enddo |
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| 171 | enddo |
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| 172 | |
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| 173 | c---------------------------------------------------------------------- |
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| 174 | c 2.0 sum of band 1 and 2 of co2 contribution |
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| 175 | c --------------------------------------- |
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| 176 | |
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| 177 | do i = 0,nlaylte+1 |
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| 178 | do j = 0,nlaylte+1 |
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| 179 | do jl = 1,kdlon |
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| 180 | |
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| 181 | ksidb(jl,3,i,j)= ksidb(jl,1,i,j) + ksidb(jl,2,i,j) |
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| 182 | |
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| 183 | enddo |
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| 184 | enddo |
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| 185 | enddo |
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| 186 | |
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| 187 | c---------------------------------------------------------------------- |
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| 188 | c 3.0 Diffusion |
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| 189 | c --------- |
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| 190 | |
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| 191 | i = nlaylte+1 |
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| 192 | do jl = 1,kdlon |
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| 193 | fluxdiff(jl,1,i) = 0. |
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| 194 | fluxdiff(jl,2,i) = 0. |
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| 195 | enddo |
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| 196 | |
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| 197 | call lwdiff (kdlon,kflev |
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| 198 | . ,bsurf,btop,dbsublay |
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| 199 | . ,tautotal,omegtotal,gtotal |
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| 200 | . ,emis,fluxdiff) |
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| 201 | |
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| 202 | c---------------------------------------------------------------------- |
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| 203 | c 4.0 Radiative Budget for each layer i |
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| 204 | c --------------------------------- |
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| 205 | |
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| 206 | do i = 1,nlaylte |
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| 207 | do jl = 1,kdlon |
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| 208 | netrad(jl,i) = 0. |
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| 209 | enddo |
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| 210 | enddo |
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| 211 | |
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| 212 | do i = 1,nlaylte |
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| 213 | do j = 0,nlaylte+1 |
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| 214 | do jl = 1,kdlon |
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| 215 | |
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| 216 | netrad(jl,i) = netrad(jl,i) + ksidb(jl,3,i,j) |
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| 217 | |
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| 218 | enddo |
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| 219 | enddo |
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| 220 | enddo |
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| 221 | c diffusion contribution |
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| 222 | c ---------------------- |
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| 223 | do i = 1,nlaylte |
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| 224 | do jl = 1,kdlon |
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| 225 | |
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| 226 | netrad(jl,i) = netrad(jl,i) |
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| 227 | . - fluxdiff(jl,1,i+1) - fluxdiff(jl,2,i+1) |
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| 228 | . + fluxdiff(jl,1,i) + fluxdiff(jl,2,i) |
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| 229 | |
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| 230 | enddo |
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| 231 | enddo |
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| 232 | |
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| 233 | c---------------------------------------------------------------------- |
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| 234 | c 4.0 cooling rate for each layer i |
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| 235 | c ----------------------------- |
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| 236 | |
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| 237 | do i = 1,nlaylte |
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| 238 | do jl = 1,kdlon |
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| 239 | |
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| 240 | coolrate(jl,i) = gcp * netrad(jl,i) / dp(jl,i) |
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| 241 | |
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| 242 | enddo |
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| 243 | enddo |
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| 244 | |
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| 245 | c---------------------------------------------------------------------- |
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| 246 | c 5.0 downward flux (all layers --> ground): "fluxground" |
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| 247 | c --------------------------------------------------- |
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| 248 | |
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| 249 | do jl = 1,kdlon |
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| 250 | fluxground(jl) = 0. |
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| 251 | enddo |
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| 252 | |
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| 253 | do i = 1,nlaylte |
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| 254 | do ja = 1,nuco2 |
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| 255 | do jl = 1,kdlon |
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| 256 | |
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| 257 | fluxground(jl) = fluxground(jl) |
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| 258 | . + xi(ig0+jl,ja,0,i) * (blay(jl,ja,i)) |
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| 259 | |
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| 260 | enddo |
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| 261 | enddo |
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| 262 | enddo |
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| 263 | |
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| 264 | do jl = 1,kdlon |
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| 265 | fluxground(jl) = fluxground(jl) - fluxdiff(jl,2,1) |
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| 266 | enddo |
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| 267 | |
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| 268 | c---------------------------------------------------------------------- |
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| 269 | c 6.0 outgoing flux (all layers --> space): "fluxtop" |
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| 270 | c --------------------------------------------------- |
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| 271 | |
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| 272 | do jl = 1,kdlon |
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| 273 | fluxtop(jl) = 0. |
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| 274 | enddo |
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| 275 | |
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| 276 | do i = 0,nlaylte |
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| 277 | do jl = 1,kdlon |
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| 278 | fluxtop(jl) = fluxtop(jl)- ksidb(jl,3,i,nlaylte+1) |
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| 279 | enddo |
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| 280 | enddo |
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| 281 | |
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| 282 | do jl = 1,kdlon |
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| 283 | fluxtop(jl) = fluxtop(jl) + fluxdiff(jl,1,nlaylte+1) |
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| 284 | enddo |
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| 285 | |
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| 286 | c---------------------------------------------------------------------- |
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| 287 | c 6.5 ONLY FOR DIAGNOSTIC : Compute IR flux in the atmosphere |
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| 288 | c ------------------- |
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| 289 | c The broadband fluxes (W.m-2) at every level from surface level (l=1) |
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| 290 | c up the top of the upper layer (here: l=nlaylte+1) are: |
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| 291 | c upward : flw_up(ig1d,l) ; downward : flw_dn(ig1d,j) |
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| 292 | c |
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| 293 | computeflux = .false. |
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| 294 | |
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| 295 | IF (computeflux) THEN ! not used by the GCM only for diagnostic ! |
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| 296 | c upward flux |
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| 297 | c ~~~~~~~~~~~ |
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| 298 | do i = 0,nlaylte |
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| 299 | do j = 1,nlaylte+1 |
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| 300 | do ja = 1,nuco2 |
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| 301 | do jl = 1,kdlon |
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| 302 | coefu(jl,ja,i,j) =0. |
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| 303 | do l=j,nlaylte+1 |
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| 304 | coefu(jl,ja,i,j)=coefu(jl,ja,i,j)+xi(ig0+jl,ja,l,i) |
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| 305 | end do |
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| 306 | |
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| 307 | enddo |
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| 308 | enddo |
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| 309 | enddo |
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| 310 | enddo |
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| 311 | do j = 1,nlaylte+1 |
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| 312 | do jl = 1,kdlon |
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| 313 | flw_up(jl,j) = 0. |
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| 314 | do ja = 1,nuco2 |
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| 315 | flw_up(jl,j)=flw_up(jl,j)+bsurf(jl,ja)*coefu(jl,ja,0,j) |
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| 316 | do i=1,j-1 |
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| 317 | flw_up(jl,j)=flw_up(jl,j)+blay(jl,ja,i)*coefu(jl,ja,i,j) |
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| 318 | end do |
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| 319 | end do |
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| 320 | flw_up(jl,j)=flw_up(jl,j) + fluxdiff(jl,1,j) |
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| 321 | end do |
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| 322 | end do |
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| 323 | |
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| 324 | c downward flux |
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| 325 | c ~~~~~~~~~~~~~ |
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| 326 | do i = 1,nlaylte+1 |
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| 327 | do j = 1,nlaylte+1 |
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| 328 | do ja = 1,nuco2 |
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| 329 | do jl = 1,kdlon |
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| 330 | coefd(jl,ja,i,j) =0. |
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| 331 | do l=0,j-1 |
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| 332 | coefd(jl,ja,i,j)=coefd(jl,ja,i,j)+xi(ig0+jl,ja,l,i) |
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| 333 | end do |
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| 334 | enddo |
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| 335 | enddo |
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| 336 | enddo |
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| 337 | enddo |
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| 338 | do j = 1,nlaylte+1 |
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| 339 | do jl = 1,kdlon |
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| 340 | flw_dn(jl,j) = 0. |
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| 341 | do ja = 1,nuco2 |
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| 342 | do i=j,nlaylte |
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| 343 | flw_dn(jl,j)=flw_dn(jl,j)+blay(jl,ja,i)*coefd(jl,ja,i,j) |
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| 344 | end do |
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| 345 | end do |
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| 346 | flw_dn(jl,j)=flw_dn(jl,j) - fluxdiff(jl,2,j) |
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| 347 | end do |
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| 348 | end do |
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| 349 | END IF |
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| 350 | |
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| 351 | c---------------------------------------------------------------------- |
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| 352 | c 7.0 outputs Grads 2D |
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| 353 | c ---------------- |
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| 354 | |
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| 355 | c ig1d: point de la grille physique ou on veut faire la sortie |
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| 356 | c ig0+1: point du decoupage de la grille physique |
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| 357 | |
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| 358 | if (callg2d) then |
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| 359 | |
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| [1047] | 360 | ig1d = kdlon/2 + 1 |
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| 361 | c ig1d = kdlon |
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| [38] | 362 | |
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| 363 | if ((ig0+1).LE.ig1d .and. ig1d.LE.(ig0+kdlon) |
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| [1047] | 364 | . .OR. kdlon.EQ.1 ) then |
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| [38] | 365 | |
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| 366 | ig = ig1d-ig0 |
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| 367 | print*, 'Sortie g2d: ig1d, ig, ig0', ig1d, ig, ig0 |
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| 368 | |
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| 369 | c-------------------------------------------- |
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| 370 | c Ouverture de g2d.dat |
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| 371 | c-------------------------------------------- |
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| 372 | if (g2d_premier) then |
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| 373 | open (47,file='g2d.dat' |
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| 374 | clmd & ,form='unformatted',access='direct',recl=4) |
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| 375 | & ,form='unformatted',access='direct',recl=1 |
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| 376 | & ,status='unknown') |
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| 377 | g2d_irec=0 |
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| 378 | g2d_appel=0 |
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| 379 | g2d_premier=.false. |
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| 380 | endif |
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| 381 | g2d_appel = g2d_appel+1 |
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| 382 | |
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| 383 | c-------------------------------------------- |
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| 384 | c Sortie g2d des xi proches + distants |
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| 385 | c-------------------------------------------- |
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| 386 | cl if (nflev .NE. 500) then |
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| 387 | do ja = 1,nuco2 |
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| 388 | do j = 0,nlaylte+1 |
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| 389 | do i = 0,nlaylte+1 |
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| 390 | g2d_irec=g2d_irec+1 |
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| 391 | reel4 = xi(ig1d,ja,i,j) |
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| 392 | write(47,rec=g2d_irec) reel4 |
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| 393 | enddo |
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| 394 | enddo |
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| 395 | enddo |
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| 396 | cl endif |
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| 397 | |
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| 398 | c------------------------------------------------------ |
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| 399 | c Writeg2d des ksidb |
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| 400 | c------------------------------------------------------ |
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| 401 | do ja = 1,nuco2 |
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| 402 | c ja=1 |
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| 403 | do j = 0,nlaylte+1 |
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| 404 | do i = 0,nlaylte+1 |
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| 405 | g2d_irec=g2d_irec+1 |
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| 406 | reel4 = ksidb(ig,ja,i,j) |
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| 407 | write(47,rec=g2d_irec) reel4 |
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| 408 | enddo |
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| 409 | enddo |
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| 410 | enddo |
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| 411 | |
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| 412 | do j = 0,nlaylte+1 |
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| 413 | do i = 0,nlaylte+1 |
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| 414 | g2d_irec=g2d_irec+1 |
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| 415 | reel4 = ksidb(ig,3,i,j) |
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| 416 | write(47,rec=g2d_irec) reel4 |
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| 417 | enddo |
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| 418 | enddo |
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| 419 | |
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| 420 | c------------------------------------------------------ |
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| 421 | c Writeg2d dpsgcp |
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| 422 | c------------------------------------------------------ |
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| 423 | |
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| 424 | do j = 1 , nlaylte |
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| 425 | do i = 0 , nlaylte+1 |
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| 426 | dpsgcp(i,j) = dp(ig,j) / gcp |
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| 427 | enddo |
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| 428 | enddo |
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| 429 | |
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| 430 | do i = 0 , nlaylte+1 |
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| 431 | c dpsgcp(i,0) = 0.0002 ! (rapport ~ entre 1000 et 10000 pour le sol) |
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| 432 | dpsgcp(i,0) = 1. ! (pour regler l'echelle des sorties) |
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| 433 | dpsgcp(i,nlaylte+1) = 0. |
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| 434 | enddo |
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| 435 | |
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| 436 | c print* |
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| 437 | c print*,'gcp: ',gcp |
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| 438 | c print* |
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| 439 | c do i = 0 , nlaylte+1 |
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| 440 | c print*,i,'dp: ',dp(ig,i) |
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| 441 | c enddo |
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| 442 | c print* |
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| 443 | c do i = 0 , nlaylte+1 |
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| 444 | c print*,i,'dpsgcp: ',dpsgcp(i,1) |
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| 445 | c enddo |
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| 446 | |
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| 447 | do j = 0,nlaylte+1 |
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| 448 | do i = 0,nlaylte+1 |
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| 449 | g2d_irec=g2d_irec+1 |
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| 450 | reel4 = dpsgcp(i,j) |
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| 451 | write(47,rec=g2d_irec) reel4 |
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| 452 | enddo |
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| 453 | enddo |
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| 454 | |
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| 455 | c------------------------------------------------------ |
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| 456 | c Writeg2d temperature |
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| 457 | c------------------------------------------------------ |
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| 458 | |
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| 459 | do j = 1 , nlaylte |
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| 460 | do i = 0 , nlaylte+1 |
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| 461 | temp(i,j) = tlay(ig,j) |
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| 462 | enddo |
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| 463 | enddo |
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| 464 | |
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| 465 | do i = 0 , nlaylte+1 |
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| 466 | temp(i,0) = tlev(ig,1)+dt0(ig) ! temperature surface |
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| 467 | temp(i,nlaylte+1) = 0. ! temperature espace (=0) |
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| 468 | enddo |
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| 469 | |
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| 470 | do j = 0,nlaylte+1 |
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| 471 | do i = 0,nlaylte+1 |
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| 472 | g2d_irec=g2d_irec+1 |
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| 473 | reel4 = temp(i,j) |
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| 474 | write(47,rec=g2d_irec) reel4 |
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| 475 | enddo |
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| 476 | enddo |
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| 477 | |
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| 478 | write(76,*) 'ig1d, ig, ig0', ig1d, ig, ig0 |
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| 479 | write(76,*) 'nlaylte', nlaylte |
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| 480 | write(76,*) 'nflev', nflev |
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| 481 | write(76,*) 'kdlon', kdlon |
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| 482 | write(76,*) 'ndlo2', ndlo2 |
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| 483 | write(76,*) 'ndlon', ndlon |
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| 484 | do ja=1,4 |
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| 485 | write(76,*) 'bsurf', ja, bsurf(ig,ja) |
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| 486 | write(76,*) 'btop', ja, btop(ig,ja) |
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| 487 | |
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| 488 | do j=1,nlaylte+1 |
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| 489 | write(76,*) 'blev', ja, j, blev(ig,ja,j) |
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| 490 | enddo |
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| 491 | |
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| 492 | do j=1,nlaylte |
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| 493 | write(76,*) 'blay', ja, j, blay(ig,ja,j) |
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| 494 | enddo |
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| 495 | |
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| 496 | do j=1,2*nlaylte |
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| 497 | write(76,*) 'dbsublay', ja, j, dbsublay(ig,ja,j) |
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| 498 | enddo |
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| 499 | enddo |
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| 500 | |
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| 501 | endif |
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| 502 | c************************************************************************ |
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| 503 | endif ! callg2d |
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| 504 | |
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| 505 | end |
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