[2032] | 1 | MODULE optcv_mod |
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| 2 | |
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| 3 | IMPLICIT NONE |
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| 4 | |
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| 5 | CONTAINS |
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| 6 | |
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[716] | 7 | SUBROUTINE OPTCV(DTAUV,TAUV,TAUCUMV,PLEV, & |
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| 8 | QXVAER,QSVAER,GVAER,WBARV,COSBV, & |
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| 9 | TAURAY,TAUAERO,TMID,PMID,TAUGSURF,QVAR,MUVAR) |
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[253] | 10 | |
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[2032] | 11 | use radinc_h, only: L_NLAYRAD, L_NLEVRAD, L_LEVELS, L_NSPECTV, L_NGAUSS, L_REFVAR, NAERKIND |
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[1194] | 12 | use radcommon_h, only: gasv, tlimit, wrefVAR, Cmk, tgasref, pfgasref,wnov,scalep,indv,glat_ig |
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[2032] | 13 | use gases_h, only: gfrac, ngasmx, igas_H2, igas_H2O, igas_He, igas_N2 |
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[1384] | 14 | use comcstfi_mod, only: g, r, mugaz |
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[1397] | 15 | use callkeys_mod, only: kastprof,continuum,graybody,H2Ocont_simple,callgasvis |
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[253] | 16 | |
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[716] | 17 | implicit none |
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[253] | 18 | |
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[716] | 19 | !================================================================== |
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| 20 | ! |
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| 21 | ! Purpose |
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| 22 | ! ------- |
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| 23 | ! Calculates shortwave optical constants at each level. |
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| 24 | ! |
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| 25 | ! Authors |
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| 26 | ! ------- |
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| 27 | ! Adapted from the NASA Ames code by R. Wordsworth (2009) |
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| 28 | ! |
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| 29 | !================================================================== |
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| 30 | ! |
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| 31 | ! THIS SUBROUTINE SETS THE OPTICAL CONSTANTS IN THE VISUAL |
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[1715] | 32 | ! IT CALCULATES FOR EACH LAYER, FOR EACH SPECTRAL INTERVAL IN THE VISUAL |
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[716] | 33 | ! LAYER: WBAR, DTAU, COSBAR |
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| 34 | ! LEVEL: TAU |
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| 35 | ! |
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| 36 | ! TAUV(L,NW,NG) is the cumulative optical depth at the top of radiation code |
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| 37 | ! layer L. NW is spectral wavelength interval, ng the Gauss point index. |
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| 38 | ! |
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| 39 | ! TLEV(L) - Temperature at the layer boundary |
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| 40 | ! PLEV(L) - Pressure at the layer boundary (i.e. level) |
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| 41 | ! GASV(NT,NPS,NW,NG) - Visible k-coefficients |
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| 42 | ! |
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| 43 | !------------------------------------------------------------------- |
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[253] | 44 | |
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| 45 | |
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[716] | 46 | real*8 DTAUV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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[1715] | 47 | real*8 DTAUKV(L_LEVELS,L_NSPECTV,L_NGAUSS) |
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[716] | 48 | real*8 TAUV(L_NLEVRAD,L_NSPECTV,L_NGAUSS) |
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| 49 | real*8 TAUCUMV(L_LEVELS,L_NSPECTV,L_NGAUSS) |
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| 50 | real*8 PLEV(L_LEVELS) |
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| 51 | real*8 TMID(L_LEVELS), PMID(L_LEVELS) |
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| 52 | real*8 COSBV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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| 53 | real*8 WBARV(L_NLAYRAD,L_NSPECTV,L_NGAUSS) |
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[253] | 54 | |
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[716] | 55 | ! for aerosols |
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[1715] | 56 | real*8 QXVAER(L_LEVELS,L_NSPECTV,NAERKIND) |
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| 57 | real*8 QSVAER(L_LEVELS,L_NSPECTV,NAERKIND) |
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| 58 | real*8 GVAER(L_LEVELS,L_NSPECTV,NAERKIND) |
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| 59 | real*8 TAUAERO(L_LEVELS,NAERKIND) |
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| 60 | real*8 TAUAEROLK(L_LEVELS,L_NSPECTV,NAERKIND) |
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[873] | 61 | real*8 TAEROS(L_LEVELS,L_NSPECTV,NAERKIND) |
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[253] | 62 | |
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[873] | 63 | integer L, NW, NG, K, LK, IAER |
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[716] | 64 | integer MT(L_LEVELS), MP(L_LEVELS), NP(L_LEVELS) |
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| 65 | real*8 ANS, TAUGAS |
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[873] | 66 | real*8 TAURAY(L_NSPECTV) |
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[716] | 67 | real*8 TRAY(L_LEVELS,L_NSPECTV) |
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| 68 | real*8 DPR(L_LEVELS), U(L_LEVELS) |
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| 69 | real*8 LCOEF(4), LKCOEF(L_LEVELS,4) |
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[253] | 70 | |
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[873] | 71 | real*8 taugsurf(L_NSPECTV,L_NGAUSS-1) |
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[918] | 72 | real*8 DCONT,DAERO |
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[1715] | 73 | real*8 DRAYAER |
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[873] | 74 | double precision wn_cont, p_cont, p_air, T_cont, dtemp, dtempc |
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| 75 | double precision p_cross |
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[253] | 76 | |
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[716] | 77 | ! variable species mixing ratio variables |
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[873] | 78 | real*8 QVAR(L_LEVELS), WRATIO(L_LEVELS), MUVAR(L_LEVELS) |
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| 79 | real*8 KCOEF(4) |
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[716] | 80 | integer NVAR(L_LEVELS) |
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[1725] | 81 | |
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| 82 | ! temporary variables to reduce memory access time to gasv |
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| 83 | real*8 tmpk(2,2) |
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| 84 | real*8 tmpkvar(2,2,2) |
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[253] | 85 | |
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[716] | 86 | ! temporary variables for multiple aerosol calculation |
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[918] | 87 | real*8 atemp(L_NLAYRAD,L_NSPECTV) |
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| 88 | real*8 btemp(L_NLAYRAD,L_NSPECTV) |
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| 89 | real*8 ctemp(L_NLAYRAD,L_NSPECTV) |
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[253] | 90 | |
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[716] | 91 | ! variables for k in units m^-1 |
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[873] | 92 | real*8 dz(L_LEVELS) |
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[253] | 93 | |
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[716] | 94 | integer igas, jgas |
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[253] | 95 | |
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[873] | 96 | integer interm |
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| 97 | |
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| 98 | !! AS: to save time in computing continuum (see bilinearbig) |
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| 99 | IF (.not.ALLOCATED(indv)) THEN |
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[878] | 100 | ALLOCATE(indv(L_NSPECTV,ngasmx,ngasmx)) |
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[873] | 101 | indv = -9999 ! this initial value means "to be calculated" |
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| 102 | ENDIF |
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| 103 | |
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[716] | 104 | !======================================================================= |
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| 105 | ! Determine the total gas opacity throughout the column, for each |
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| 106 | ! spectral interval, NW, and each Gauss point, NG. |
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| 107 | ! Calculate the continuum opacities, i.e., those that do not depend on |
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| 108 | ! NG, the Gauss index. |
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[253] | 109 | |
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[716] | 110 | taugsurf(:,:) = 0.0 |
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| 111 | dpr(:) = 0.0 |
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| 112 | lkcoef(:,:) = 0.0 |
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[253] | 113 | |
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[716] | 114 | do K=2,L_LEVELS |
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| 115 | DPR(k) = PLEV(K)-PLEV(K-1) |
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[253] | 116 | |
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[716] | 117 | ! if we have continuum opacities, we need dz |
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| 118 | if(kastprof)then |
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[1016] | 119 | dz(k) = dpr(k)*(1000.0d0*8.3145d0/muvar(k))*TMID(K)/(g*PMID(K)) |
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| 120 | U(k) = Cmk*DPR(k)*mugaz/muvar(k) |
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[716] | 121 | else |
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[1194] | 122 | dz(k) = dpr(k)*R*TMID(K)/(glat_ig*PMID(K))*mugaz/muvar(k) |
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[1016] | 123 | U(k) = Cmk*DPR(k)*mugaz/muvar(k) ! only Cmk line in optci.F |
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| 124 | !JL13 the mugaz/muvar factor takes into account water meanmolecular weight if water is present |
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[716] | 125 | endif |
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[253] | 126 | |
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[716] | 127 | call tpindex(PMID(K),TMID(K),QVAR(K),pfgasref,tgasref,WREFVAR, & |
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| 128 | LCOEF,MT(K),MP(K),NVAR(K),WRATIO(K)) |
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[253] | 129 | |
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[716] | 130 | do LK=1,4 |
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| 131 | LKCOEF(K,LK) = LCOEF(LK) |
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| 132 | end do |
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[918] | 133 | end do ! levels |
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[253] | 134 | |
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[1715] | 135 | ! Spectral dependance of aerosol absorption |
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[1987] | 136 | !JL18 It seems to be good to have aerosols in the first "radiative layer" of the gcm in the IR |
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| 137 | ! but visible does not handle very well diffusion in first layer. |
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| 138 | ! The tauaero and tauray are thus set to 0 (a small value for rayleigh because the code crashes otherwise) |
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| 139 | ! in the 4 first semilayers in optcv, but not optci. |
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| 140 | ! This solves random variations of the sw heating at the model top. |
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[918] | 141 | do iaer=1,naerkind |
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| 142 | do NW=1,L_NSPECTV |
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[1987] | 143 | TAEROS(1:4,NW,IAER)=0.d0 |
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| 144 | do K=5,L_LEVELS |
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[873] | 145 | TAEROS(K,NW,IAER) = TAUAERO(K,IAER) * QXVAER(K,NW,IAER) |
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[918] | 146 | end do ! levels |
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| 147 | end do |
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| 148 | end do |
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[1715] | 149 | |
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| 150 | ! Rayleigh scattering |
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[918] | 151 | do NW=1,L_NSPECTV |
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[1987] | 152 | TRAY(1:4,NW) = 1d-30 |
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| 153 | do K=5,L_LEVELS |
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[873] | 154 | TRAY(K,NW) = TAURAY(NW) * DPR(K) |
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[918] | 155 | end do ! levels |
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| 156 | end do |
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| 157 | |
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[716] | 158 | ! we ignore K=1... |
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| 159 | do K=2,L_LEVELS |
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[873] | 160 | |
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[716] | 161 | do NW=1,L_NSPECTV |
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[253] | 162 | |
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[1715] | 163 | DRAYAER = TRAY(K,NW) |
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| 164 | ! DRAYAER is Tau RAYleigh scattering, plus AERosol opacity |
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[716] | 165 | do iaer=1,naerkind |
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[1715] | 166 | DRAYAER = DRAYAER + TAEROS(K,NW,IAER) |
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[716] | 167 | end do |
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[253] | 168 | |
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[716] | 169 | DCONT = 0.0 ! continuum absorption |
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[253] | 170 | |
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[873] | 171 | if(continuum.and.(.not.graybody).and.callgasvis)then |
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[716] | 172 | ! include continua if necessary |
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| 173 | wn_cont = dble(wnov(nw)) |
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| 174 | T_cont = dble(TMID(k)) |
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| 175 | do igas=1,ngasmx |
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[305] | 176 | |
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[716] | 177 | if(gfrac(igas).eq.-1)then ! variable |
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| 178 | p_cont = dble(PMID(k)*scalep*QVAR(k)) ! qvar = mol/mol |
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| 179 | else |
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| 180 | p_cont = dble(PMID(k)*scalep*gfrac(igas)*(1.-QVAR(k))) |
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| 181 | endif |
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[305] | 182 | |
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[716] | 183 | dtemp=0.0 |
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| 184 | if(igas.eq.igas_N2)then |
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[253] | 185 | |
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[878] | 186 | interm = indv(nw,igas,igas) |
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| 187 | ! call interpolateN2N2(wn_cont,T_cont,p_cont,dtemp,.false.,interm) |
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| 188 | indv(nw,igas,igas) = interm |
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[716] | 189 | ! only goes to 500 cm^-1, so unless we're around a cold brown dwarf, this is irrelevant in the visible |
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[253] | 190 | |
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[716] | 191 | elseif(igas.eq.igas_H2)then |
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[253] | 192 | |
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[716] | 193 | ! first do self-induced absorption |
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[878] | 194 | interm = indv(nw,igas,igas) |
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[873] | 195 | call interpolateH2H2(wn_cont,T_cont,p_cont,dtemp,.false.,interm) |
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[878] | 196 | indv(nw,igas,igas) = interm |
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[253] | 197 | |
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[716] | 198 | ! then cross-interactions with other gases |
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| 199 | do jgas=1,ngasmx |
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| 200 | p_cross = dble(PMID(k)*scalep*gfrac(jgas)*(1.-QVAR(k))) |
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[873] | 201 | dtempc = 0.0 |
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| 202 | if(jgas.eq.igas_N2)then |
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[878] | 203 | interm = indv(nw,igas,jgas) |
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| 204 | call interpolateN2H2(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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| 205 | indv(nw,igas,jgas) = interm |
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[716] | 206 | ! should be irrelevant in the visible |
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| 207 | elseif(jgas.eq.igas_He)then |
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[878] | 208 | interm = indv(nw,igas,jgas) |
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[873] | 209 | call interpolateH2He(wn_cont,T_cont,p_cross,p_cont,dtempc,.false.,interm) |
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[878] | 210 | indv(nw,igas,jgas) = interm |
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[716] | 211 | endif |
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[873] | 212 | dtemp = dtemp + dtempc |
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[716] | 213 | enddo |
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[253] | 214 | |
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[716] | 215 | elseif(igas.eq.igas_H2O.and.T_cont.gt.200.0)then |
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[253] | 216 | |
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[716] | 217 | p_air = dble(PMID(k)*scalep) - p_cont ! note assumes background is air! |
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| 218 | if(H2Ocont_simple)then |
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| 219 | call interpolateH2Ocont_PPC(wn_cont,T_cont,p_cont,p_air,dtemp,.false.) |
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| 220 | else |
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[878] | 221 | interm = indv(nw,igas,igas) |
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| 222 | call interpolateH2Ocont_CKD(wn_cont,T_cont,p_cont,p_air,dtemp,.false.,interm) |
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| 223 | indv(nw,igas,igas) = interm |
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[716] | 224 | endif |
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[253] | 225 | |
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[716] | 226 | endif |
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[253] | 227 | |
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[716] | 228 | DCONT = DCONT + dtemp |
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[253] | 229 | |
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[716] | 230 | enddo |
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[253] | 231 | |
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[873] | 232 | DCONT = DCONT*dz(k) |
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| 233 | |
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[716] | 234 | endif |
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[253] | 235 | |
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[873] | 236 | do ng=1,L_NGAUSS-1 |
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[305] | 237 | |
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[873] | 238 | ! Now compute TAUGAS |
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[253] | 239 | |
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[873] | 240 | ! Interpolate between water mixing ratios |
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| 241 | ! WRATIO = 0.0 if the requested water amount is equal to, or outside the |
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| 242 | ! the water data range |
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| 243 | |
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| 244 | if(L_REFVAR.eq.1)then ! added by RW for special no variable case |
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[1725] | 245 | |
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| 246 | ! JVO 2017 : added tmpk because the repeated calls to gasi/v increased dramatically |
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| 247 | ! the execution time of optci/v -> ~ factor 2 on the whole radiative |
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| 248 | ! transfer on the tested simulations ! |
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| 249 | |
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| 250 | tmpk = GASV(MT(K):MT(K)+1,MP(K):MP(K)+1,1,NW,NG) |
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| 251 | |
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| 252 | KCOEF(1) = tmpk(1,1) ! KCOEF(1) = GASV(MT(K),MP(K),1,NW,NG) |
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| 253 | KCOEF(2) = tmpk(1,2) ! KCOEF(2) = GASV(MT(K),MP(K)+1,1,NW,NG) |
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| 254 | KCOEF(3) = tmpk(2,2) ! KCOEF(3) = GASV(MT(K)+1,MP(K)+1,1,NW,NG) |
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| 255 | KCOEF(4) = tmpk(2,1) ! KCOEF(4) = GASV(MT(K)+1,MP(K),1,NW,NG) |
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| 256 | |
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[716] | 257 | else |
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[873] | 258 | |
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[1725] | 259 | tmpkvar = GASV(MT(K):MT(K)+1,MP(K):MP(K)+1,NVAR(K):NVAR(K)+1,NW,NG) |
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[253] | 260 | |
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[1725] | 261 | KCOEF(1) = tmpkvar(1,1,1) + WRATIO(K) * & |
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| 262 | ( tmpkvar(1,1,2)-tmpkvar(1,1,1) ) |
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[253] | 263 | |
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[1725] | 264 | KCOEF(2) = tmpkvar(1,2,1) + WRATIO(K) * & |
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| 265 | ( tmpkvar(1,2,2)-tmpkvar(1,2,1) ) |
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[253] | 266 | |
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[1725] | 267 | KCOEF(3) = tmpkvar(2,2,1) + WRATIO(K) * & |
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| 268 | ( tmpkvar(2,2,2)-tmpkvar(2,2,1) ) |
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| 269 | |
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| 270 | KCOEF(4) = tmpkvar(2,1,1) + WRATIO(K) * & |
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| 271 | ( tmpkvar(2,1,2)-tmpkvar(2,1,1) ) |
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[873] | 272 | |
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[1725] | 273 | |
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[716] | 274 | endif |
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[253] | 275 | |
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[873] | 276 | ! Interpolate the gaseous k-coefficients to the requested T,P values |
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[253] | 277 | |
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[873] | 278 | ANS = LKCOEF(K,1)*KCOEF(1) + LKCOEF(K,2)*KCOEF(2) + & |
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[716] | 279 | LKCOEF(K,3)*KCOEF(3) + LKCOEF(K,4)*KCOEF(4) |
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[253] | 280 | |
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[873] | 281 | TAUGAS = U(k)*ANS |
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[253] | 282 | |
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[716] | 283 | TAUGSURF(NW,NG) = TAUGSURF(NW,NG) + TAUGAS + DCONT |
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[873] | 284 | DTAUKV(K,nw,ng) = TAUGAS & |
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[1715] | 285 | + DRAYAER & ! DRAYAER includes all scattering contributions |
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[873] | 286 | + DCONT ! For parameterized continuum aborption |
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[253] | 287 | |
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[716] | 288 | end do |
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[253] | 289 | |
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[873] | 290 | ! Now fill in the "clear" part of the spectrum (NG = L_NGAUSS), |
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| 291 | ! which holds continuum opacity only |
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[253] | 292 | |
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[873] | 293 | NG = L_NGAUSS |
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[1715] | 294 | DTAUKV(K,nw,ng) = DRAYAER + DCONT ! Scattering + parameterized continuum absorption |
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[253] | 295 | |
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[716] | 296 | end do |
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| 297 | end do |
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[253] | 298 | |
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| 299 | |
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[716] | 300 | !======================================================================= |
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| 301 | ! Now the full treatment for the layers, where besides the opacity |
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| 302 | ! we need to calculate the scattering albedo and asymmetry factors |
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[253] | 303 | |
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[1987] | 304 | !JL18 It seems to be good to have aerosols in the first "radiative layer" of the gcm in the IR |
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| 305 | ! but not in the visible |
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| 306 | ! The tauaero is thus set to 0 in the 4 first semilayers in optcv, but not optci. |
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| 307 | ! This solves random variations of the sw heating at the model top. |
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[873] | 308 | do iaer=1,naerkind |
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[918] | 309 | DO NW=1,L_NSPECTV |
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[1987] | 310 | TAUAEROLK(1:4,NW,IAER)=0.d0 |
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| 311 | DO K=5,L_LEVELS |
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[1715] | 312 | TAUAEROLK(K,NW,IAER) = TAUAERO(K,IAER) * QSVAER(K,NW,IAER) ! effect of scattering albedo |
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[918] | 313 | ENDDO |
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| 314 | ENDDO |
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[873] | 315 | end do |
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[253] | 316 | |
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[716] | 317 | DO NW=1,L_NSPECTV |
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[919] | 318 | DO L=1,L_NLAYRAD-1 |
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[918] | 319 | K = 2*L+1 |
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| 320 | atemp(L,NW) = SUM(GVAER(K,NW,1:naerkind) * TAUAEROLK(K,NW,1:naerkind))+SUM(GVAER(K+1,NW,1:naerkind) * TAUAEROLK(K+1,NW,1:naerkind)) |
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| 321 | btemp(L,NW) = SUM(TAUAEROLK(K,NW,1:naerkind)) + SUM(TAUAEROLK(K+1,NW,1:naerkind)) |
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[1715] | 322 | ctemp(L,NW) = btemp(L,NW) + 0.9999*(TRAY(K,NW) + TRAY(K+1,NW)) ! JVO 2017 : does this 0.999 is really meaningful ? |
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[918] | 323 | btemp(L,NW) = btemp(L,NW) + TRAY(K,NW) + TRAY(K+1,NW) |
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| 324 | COSBV(L,NW,1:L_NGAUSS) = atemp(L,NW)/btemp(L,NW) |
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| 325 | END DO ! L vertical loop |
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[919] | 326 | |
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[1715] | 327 | ! Last level |
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| 328 | L = L_NLAYRAD |
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| 329 | K = 2*L+1 |
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| 330 | atemp(L,NW) = SUM(GVAER(K,NW,1:naerkind) * TAUAEROLK(K,NW,1:naerkind)) |
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[919] | 331 | btemp(L,NW) = SUM(TAUAEROLK(K,NW,1:naerkind)) |
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[1715] | 332 | ctemp(L,NW) = btemp(L,NW) + 0.9999*TRAY(K,NW) ! JVO 2017 : does this 0.999 is really meaningful ? |
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[919] | 333 | btemp(L,NW) = btemp(L,NW) + TRAY(K,NW) |
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| 334 | COSBV(L,NW,1:L_NGAUSS) = atemp(L,NW)/btemp(L,NW) |
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| 335 | |
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| 336 | |
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[918] | 337 | END DO ! NW spectral loop |
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| 338 | |
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| 339 | DO NG=1,L_NGAUSS |
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| 340 | DO NW=1,L_NSPECTV |
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[873] | 341 | DO L=1,L_NLAYRAD-1 |
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[253] | 342 | |
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[873] | 343 | K = 2*L+1 |
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| 344 | DTAUV(L,nw,ng) = DTAUKV(K,NW,NG) + DTAUKV(K+1,NW,NG) |
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[918] | 345 | WBARV(L,nw,ng) = ctemp(L,NW) / DTAUV(L,nw,ng) |
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[253] | 346 | |
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[873] | 347 | END DO ! L vertical loop |
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[253] | 348 | |
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[1715] | 349 | ! Last level |
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[253] | 350 | |
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[716] | 351 | L = L_NLAYRAD |
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| 352 | K = 2*L+1 |
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[919] | 353 | DTAUV(L,nw,ng) = DTAUKV(K,NW,NG) |
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| 354 | |
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| 355 | WBARV(L,NW,NG) = ctemp(L,NW) / DTAUV(L,NW,NG) |
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[1722] | 356 | |
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[918] | 357 | END DO ! NW spectral loop |
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| 358 | END DO ! NG Gauss loop |
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[716] | 359 | |
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| 360 | ! Total extinction optical depths |
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| 361 | |
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[918] | 362 | DO NG=1,L_NGAUSS ! full gauss loop |
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| 363 | DO NW=1,L_NSPECTV |
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[716] | 364 | TAUCUMV(1,NW,NG)=0.0D0 |
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| 365 | DO K=2,L_LEVELS |
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| 366 | TAUCUMV(K,NW,NG)=TAUCUMV(K-1,NW,NG)+DTAUKV(K,NW,NG) |
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| 367 | END DO |
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[1987] | 368 | |
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[2004] | 369 | DO L=1,L_NLAYRAD |
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[1987] | 370 | TAUV(L,NW,NG)=TAUCUMV(2*L,NW,NG) |
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| 371 | END DO |
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[2004] | 372 | TAUV(L,NW,NG)=TAUCUMV(2*L_NLAYRAD+1,NW,NG) |
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[918] | 373 | END DO |
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| 374 | END DO ! end full gauss loop |
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[716] | 375 | |
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| 376 | |
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[2032] | 377 | end subroutine optcv |
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[873] | 378 | |
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[2032] | 379 | END MODULE optcv_mod |
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