| 1 | MODULE callradite_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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| 7 | SUBROUTINE callradite(icount,ngrid,nlayer,nq,zday,ls,pq,albedo, |
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| 8 | $ emis,mu0,pplev,pplay,pt,tsurf,fract,dist_sol,igout, |
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| 9 | $ dtlw,dtsw,fluxsurf_lw,fluxsurf_sw,fluxtop_lw, |
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| 10 | $ fluxtop_sw,tau_pref_scenario,tau_pref_gcm, |
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| 11 | & tau,aerosol,dsodust,tauscaling,dust_rad_adjust, |
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| 12 | $ taucloudtes,rdust,rice,nuice,riceco2,nuiceco2,co2ice, |
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| 13 | $ rstormdust,rtopdust,totstormfract,clearatm,dsords,dsotop, |
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| 14 | $ alpha_hmons,nohmons,clearsky,totcloudfrac) |
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| 15 | |
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| 16 | use aeropacity_mod, only: aeropacity |
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| 17 | use updatereffrad_mod, only: updatereffrad |
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| 18 | use dimradmars_mod, only: ndomainsz, nflev, nsun, nir |
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| 19 | use dimradmars_mod, only: naerkind, name_iaer, |
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| 20 | & iaer_dust_conrath,iaer_dust_doubleq, |
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| 21 | & iaer_dust_submicron, iaer_h2o_ice, iaer_co2_ice, |
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| 22 | & iaer_stormdust_doubleq,iaer_topdust_doubleq |
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| 23 | use yomlw_h, only: gcp, nlaylte |
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| 24 | use comcstfi_h, only: g,cpp |
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| 25 | use time_phylmdz_mod, only: daysec |
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| 26 | use lwmain_mod, only: lwmain |
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| 27 | use swmain_mod, only: swmain |
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| 28 | use dust_param_mod, only: doubleq, active, submicron |
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| 29 | IMPLICIT NONE |
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| 30 | c======================================================================= |
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| 31 | c subject: |
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| 32 | c -------- |
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| 33 | c Subroutine designed to call the main canonic |
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| 34 | c radiative transfer subroutine "lwmain" et "swmain" |
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| 35 | c to compute radiative heating and cooling rate and |
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| 36 | c radiative fluxes to the surface. |
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| 37 | c |
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| 38 | c These calculations are only valid on the part of the atmosphere |
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| 39 | c where Local Thermal Equilibrium (LTE) is verified. In practice |
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| 40 | c the calculations are only performed for the first "nlaylte" |
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| 41 | c parameters (nlaylte is calculated by subroutine "nlthermeq" |
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| 42 | c and stored in module "yomlw_h"). |
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| 43 | c |
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| 44 | c The purpose of this subroutine is to: |
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| 45 | c 1) Make some initial calculation at first call |
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| 46 | c 2) Split the calculation in several sub-grid |
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| 47 | c ("sub-domain") to save memory and |
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| 48 | c be able run on a workstation at high resolution |
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| 49 | c The sub-grid size is defined in dimradmars_mod |
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| 50 | c 3) Compute the 3D scattering parameters depending on the |
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| 51 | c size distribution of the different tracers (added by JBM) |
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| 52 | c 4) call "lwmain" and "swmain" |
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| 53 | c |
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| 54 | c |
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| 55 | c authors: |
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| 56 | c ------ |
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| 57 | c Francois Forget / Christophe Hourdin / J.-B. Madeleine (2009) |
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| 58 | c |
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| 59 | c |
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| 60 | c 3D scattering scheme user's guide (J.-B. Madeleine) |
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| 61 | c --------------------------------- |
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| 62 | c |
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| 63 | c This routine has been modified to take into account 3D, time |
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| 64 | c dependent scattering properties of the aerosols. |
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| 65 | c---- The look-up tables that contain the scattering parameters |
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| 66 | c of a given tracer, for different sizes, are read by SUAER.F90. |
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| 67 | c The names of the corresponding ASCII files have to be set in |
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| 68 | c this subroutine (file_id variable), and files must be in the |
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| 69 | c directory specified in datafile_mod. Please make sure that the |
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| 70 | c ASCII files are correctly written, and that the range |
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| 71 | c of particle sizes is consistent with what you would expect. |
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| 72 | c---- SUAER.F90 is in charge of reading the ASCII files and averaging |
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| 73 | c the scattering parameters in each GCM channel, using the three last |
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| 74 | c equations of Forget et al. 1998 (GRL 25, No.7, p.1105-1108). |
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| 75 | c---- These look-up tables, loaded during the firstcall, are then |
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| 76 | c constantly used by the subroutine "aeroptproperties.F" to compute, |
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| 77 | c online, the 3D scattering parameters, based on the size distribution |
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| 78 | c (reffrad and nueffrad) of the different tracers, in each grid box. |
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| 79 | c These 3D size distributions are loaded by the "updatereffrad.F" |
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| 80 | c subroutine. A log-normal distribution is then assumed in |
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| 81 | c "aeroptproperties.F", along with a Gauss-Legendre integration. |
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| 82 | c---- The optical depth at the visible reference wavelength (set in |
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| 83 | c SUAER.F90, after the file_id variable) is then computed by |
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| 84 | c the subroutine "aeropacity.F", by using the size and spatial |
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| 85 | c distribution of the corresponding tracer. This connection has to |
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| 86 | c be implemented in "aeropacity.F" when adding a new tracer. To do so, |
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| 87 | c one can use equation 2 of Forget et al. 1998 (Icarus 131, p.302-316). |
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| 88 | c---- The resulting variables "aerosol", "QVISsQREF3d", "omegaVIS3d" and |
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| 89 | c "gVIS3d" (same in the infrared) are finally used by lwmain.F and |
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| 90 | c swmain.F to solve the radiative transfer equation. |
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| 91 | c |
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| 92 | c changes: |
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| 93 | c ------- |
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| 94 | c |
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| 95 | c > SRL 7/2000 |
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| 96 | c |
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| 97 | c This version has been modified to only calculate radiative tendencies |
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| 98 | c over layers 1..NFLEV (set in dimradmars_mod). Returns zero for higher |
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| 99 | c layers, if any. |
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| 100 | c In other routines, nlayer -> nflev. |
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| 101 | c Routines affected: lwflux, lwi, lwmain, lwxb, lwxd, lwxn. |
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| 102 | c |
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| 103 | c > J.-B. Madeleine 10W12 |
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| 104 | c This version uses the variable's splitting, which can be usefull |
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| 105 | c when performing very high resolution simulation like LES. |
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| 106 | c |
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| 107 | c ---------- |
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| 108 | c Here, solar band#1 is spectral interval between "long1vis" and "long2vis" |
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| 109 | c set in dimradmars_mod |
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| 110 | c Here, solar band#2 is spectral interval between "long2vis" and "long3vis" |
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| 111 | c set in dimradmars_mod |
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| 112 | c |
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| 113 | c input: |
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| 114 | c ----- |
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| 115 | c icount counter of call to subroutine physic by gcm |
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| 116 | c ngrid number of gridpoint of horizontal grid |
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| 117 | c nlayer Number of layer |
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| 118 | c nq Number of tracer |
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| 119 | c ls Solar longitude (Ls) , radian |
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| 120 | c zday Date (time since Ls=0, in martian days) |
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| 121 | c pq(ngrid,nlayer,nq) Advected fields |
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| 122 | c |
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| 123 | c albedo (ngrid,2) hemispheric surface albedo |
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| 124 | c albedo (i,1) : mean albedo for solar band#1 |
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| 125 | c (see below) |
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| 126 | c albedo (i,2) : mean albedo for solar band#2 |
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| 127 | c (see below) |
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| 128 | c emis Thermal IR surface emissivity (no unit) |
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| 129 | c mu0(ngrid) cos of solar zenith angle |
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| 130 | c (=1 when sun at zenith) |
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| 131 | c pplay(ngrid,nlayer) pressure (Pa) in the middle of each layer |
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| 132 | c pplev(ngrid,nlayer+1) pressure (Pa) at boundaries of each layer |
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| 133 | c pt(ngrid,nlayer) atmospheric temperature in each layer (K) |
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| 134 | c tsurf(ngrid) surface temperature (K) |
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| 135 | c fract(ngrid) day fraction of the time interval |
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| 136 | c =1 during the full day ; =0 during the night |
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| 137 | c declin latitude of subsolar point |
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| 138 | c dist_sol sun-Mars distance (AU) |
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| 139 | c igout coordinate of analysed point for debugging |
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| 140 | c reffrad(ngrid,nlayer,naerkind) Aerosol effective radius |
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| 141 | c nueffrad(ngrid,nlayer,naerkind) Aerosol effective variance |
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| 142 | |
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| 143 | c |
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| 144 | c output: |
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| 145 | c ------- |
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| 146 | c dtlw (ngrid,nlayer) longwave (IR) heating rate (K/s) |
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| 147 | c dtsw(ngrid,nlayer) shortwave (Solar) heating rate (K/s) |
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| 148 | c fluxsurf_lw(ngrid) surface downward flux tota LW (thermal IR) (W.m-2) |
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| 149 | c fluxsurf_sw(ngrid,1) surface downward flux SW for solar band#1 (W.m-2) |
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| 150 | c fluxsurf_sw(ngrid,2) surface downward flux SW for solar band#2 (W.m-2) |
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| 151 | c |
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| 152 | c fluxtop_lw(ngrid) outgoing upward flux tota LW (thermal IR) (W.m-2) |
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| 153 | c fluxtop_sw(ngrid,1) outgoing upward flux SW for solar band#1 (W.m-2) |
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| 154 | c fluxtop_sw(ngrid,2) outgoing upward flux SW for solar band#2 (W.m-2) |
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| 155 | |
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| 156 | c tau Column total visible dust optical depth at each point |
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| 157 | c aerosol(ngrid,nlayer,naerkind) aerosol extinction optical depth |
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| 158 | c at reference wavelength "longrefvis" set |
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| 159 | c in dimradmars_h , in each layer, for one of |
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| 160 | c the "naerkind" kind of aerosol optical |
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| 161 | c properties. |
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| 162 | c======================================================================= |
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| 163 | c |
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| 164 | c Declarations : |
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| 165 | c ------------- |
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| 166 | c |
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| 167 | include "callkeys.h" |
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| 168 | |
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| 169 | c----------------------------------------------------------------------- |
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| 170 | c Input/Output |
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| 171 | c ------------ |
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| 172 | INTEGER,INTENT(IN) :: icount |
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| 173 | INTEGER,INTENT(IN) :: ngrid,nlayer,nq |
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| 174 | INTEGER,INTENT(IN) :: igout |
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| 175 | |
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| 176 | REAL,INTENT(IN) :: pq(ngrid,nlayer,nq) |
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| 177 | REAL,INTENT(INOUT) :: tauscaling(ngrid) ! Conversion factor for |
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| 178 | ! qdust and Ndust |
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| 179 | REAL,INTENT(OUT) :: dust_rad_adjust(ngrid) ! Radiative adjustment |
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| 180 | ! factor for dust |
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| 181 | REAL,INTENT(IN) :: albedo(ngrid,2),emis(ngrid) |
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| 182 | REAL,INTENT(IN) :: ls,zday |
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| 183 | |
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| 184 | REAL,INTENT(IN) :: pplev(ngrid,nlayer+1),pplay(ngrid,nlayer) |
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| 185 | REAL,INTENT(IN) :: pt(ngrid,nlayer) |
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| 186 | REAL,INTENT(IN) :: tsurf(ngrid) |
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| 187 | REAL,INTENT(IN) :: dist_sol,mu0(ngrid),fract(ngrid) |
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| 188 | REAL,INTENT(OUT) :: dtlw(ngrid,nlayer),dtsw(ngrid,nlayer) |
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| 189 | REAL,INTENT(OUT) :: fluxsurf_lw(ngrid), fluxtop_lw(ngrid) |
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| 190 | REAL,INTENT(OUT) :: fluxsurf_sw(ngrid,2), fluxtop_sw(ngrid,2) |
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| 191 | REAL,INTENT(OUT) :: tau_pref_scenario(ngrid) ! prescribed dust column |
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| 192 | ! visible opacity at odpref from scenario |
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| 193 | REAL,INTENT(OUT) :: tau_pref_gcm(ngrid) ! computed dust column |
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| 194 | ! visible opacity at odpref in the GCM |
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| 195 | REAL,INTENT(OUT) :: tau(ngrid,naerkind) |
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| 196 | REAL,INTENT(OUT) :: taucloudtes(ngrid)! Cloud opacity at infrared |
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| 197 | ! reference wavelength using |
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| 198 | ! Qabs instead of Qext |
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| 199 | ! (direct comparison with TES) |
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| 200 | REAL,INTENT(OUT) :: aerosol(ngrid,nlayer,naerkind) |
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| 201 | REAL,INTENT(INOUT) :: dsodust(ngrid,nlayer) |
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| 202 | REAL,INTENT(OUT) :: rdust(ngrid,nlayer) ! Dust geometric mean radius (m) |
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| 203 | REAL,INTENT(OUT) :: rice(ngrid,nlayer) ! Ice geometric mean radius (m) |
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| 204 | REAL,INTENT(OUT) :: nuice(ngrid,nlayer) ! Estimated effective variance |
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| 205 | double precision,INTENT(OUT) :: riceco2(ngrid,nlayer) ! CO2 ice mean radius(m) |
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| 206 | REAL,INTENT(OUT) :: nuiceco2(ngrid,nlayer) ! Effective variance |
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| 207 | REAL,INTENT(IN) :: co2ice(ngrid) ! co2 ice surface layer (kg.m-2) |
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| 208 | |
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| 209 | c rocket dust storm |
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| 210 | LOGICAL,INTENT(IN) :: clearatm ! true for background dust |
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| 211 | REAL,INTENT(IN) :: totstormfract(ngrid) ! dust storm mesh fraction |
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| 212 | REAL,INTENT(OUT) :: rstormdust(ngrid,nlayer) ! Storm dust geometric mean radius (m) |
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| 213 | REAL,INTENT(OUT) :: dsords(ngrid,nlayer) ! density scaled opacity for rocket dust storm dust |
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| 214 | |
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| 215 | c entrainment by slope wind |
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| 216 | LOGICAL, INTENT(IN) :: nohmons ! true for background dust |
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| 217 | REAL, INTENT(IN) :: alpha_hmons(ngrid) ! sub-grid scale topography mesh fraction |
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| 218 | REAL,INTENT(OUT) :: rtopdust(ngrid,nlayer) ! Topdust geometric mean radius (m) |
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| 219 | REAL,INTENT(OUT) :: dsotop(ngrid,nlayer) ! density scaled opacity for topmons dust |
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| 220 | |
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| 221 | c sub-grid scale water ice clouds |
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| 222 | LOGICAL,INTENT(IN) :: clearsky |
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| 223 | REAL,INTENT(IN) :: totcloudfrac(ngrid) |
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| 224 | |
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| 225 | c |
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| 226 | c Local variables : |
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| 227 | c ----------------- |
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| 228 | |
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| 229 | INTEGER j,l,ig,n,ich |
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| 230 | INTEGER aer_count,iaer |
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| 231 | INTEGER jd,ig0,nd |
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| 232 | |
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| 233 | real cste_mars ! solar constant on Mars (Wm-2) |
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| 234 | REAL ptlev(ngrid,nlayer+1) |
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| 235 | |
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| 236 | INTEGER :: ndomain |
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| 237 | |
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| 238 | c Thermal IR net radiative budget (W m-2) |
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| 239 | |
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| 240 | real znetrad(ndomainsz,nflev) |
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| 241 | |
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| 242 | real zfluxd_sw(ndomainsz,nflev+1,2) |
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| 243 | real zfluxu_sw(ndomainsz,nflev+1,2) |
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| 244 | |
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| 245 | REAL zplev(ndomainsz,nflev+1) |
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| 246 | REAL zztlev(ndomainsz,nflev+1) |
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| 247 | REAL zplay(ndomainsz,nflev) |
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| 248 | REAL zt(ndomainsz,nflev) |
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| 249 | REAL zaerosol(ndomainsz,nflev,naerkind) |
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| 250 | REAL zalbedo(ndomainsz,2) |
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| 251 | REAL zdp(ndomainsz,nflev) |
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| 252 | REAL zdt0(ndomainsz) |
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| 253 | |
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| 254 | REAL zzdtlw(ndomainsz,nflev) |
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| 255 | REAL zzdtsw(ndomainsz,nflev) |
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| 256 | REAL zzflux(ndomainsz,6) |
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| 257 | real zrmuz |
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| 258 | |
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| 259 | REAL :: zQVISsQREF3d(ndomainsz,nflev,nsun,naerkind) |
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| 260 | REAL :: zomegaVIS3d(ndomainsz,nflev,nsun,naerkind) |
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| 261 | REAL :: zgVIS3d(ndomainsz,nflev,nsun,naerkind) |
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| 262 | |
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| 263 | REAL :: zQIRsQREF3d(ndomainsz,nflev,nir,naerkind) |
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| 264 | REAL :: zomegaIR3d(ndomainsz,nflev,nir,naerkind) |
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| 265 | REAL :: zgIR3d(ndomainsz,nflev,nir,naerkind) |
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| 266 | |
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| 267 | c Aerosol size distribution |
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| 268 | REAL :: reffrad(ngrid,nlayer,naerkind) |
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| 269 | REAL :: nueffrad(ngrid,nlayer,naerkind) |
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| 270 | c Aerosol optical properties |
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| 271 | REAL :: QVISsQREF3d(ngrid,nlayer,nsun,naerkind) |
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| 272 | REAL :: omegaVIS3d(ngrid,nlayer,nsun,naerkind) |
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| 273 | REAL :: gVIS3d(ngrid,nlayer,nsun,naerkind) |
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| 274 | |
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| 275 | REAL :: QIRsQREF3d(ngrid,nlayer,nir,naerkind) |
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| 276 | REAL :: omegaIR3d(ngrid,nlayer,nir,naerkind) |
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| 277 | REAL :: gIR3d(ngrid,nlayer,nir,naerkind) |
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| 278 | |
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| 279 | REAL :: QREFvis3d(ngrid,nlayer,naerkind) |
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| 280 | ! QREFvis3d : Extinction efficiency at the VISible reference wavelength |
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| 281 | REAL :: QREFir3d(ngrid,nlayer,naerkind) |
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| 282 | ! QREFir3d : Extinction efficiency at the InfraRed reference wavelength |
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| 283 | |
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| 284 | REAL :: omegaREFvis3d(ngrid,nlayer,naerkind) |
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| 285 | REAL :: omegaREFir3d(ngrid,nlayer,naerkind) |
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| 286 | |
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| 287 | c local saved variables |
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| 288 | c --------------------- |
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| 289 | |
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| 290 | real zco2 ! volume fraction of CO2 in Mars atmosphere |
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| 291 | !$OMP THREADPRIVATE(zco2) |
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| 292 | DATA zco2/0.95/ |
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| 293 | SAVE zco2 |
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| 294 | |
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| 295 | LOGICAL firstcall |
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| 296 | !$OMP THREADPRIVATE(firstcall) |
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| 297 | DATA firstcall/.true./ |
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| 298 | SAVE firstcall |
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| 299 | |
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| 300 | |
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| 301 | |
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| 302 | c---------------------------------------------------------------------- |
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| 303 | |
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| 304 | c Initialisation |
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| 305 | c -------------- |
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| 306 | |
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| 307 | ! compute ndomain |
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| 308 | ! AS: moved out of firstcall to allow nesting+evoluting domain |
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| 309 | ! ------------------------------------------------------------ |
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| 310 | ndomain= (ngrid-1) / ndomainsz + 1 |
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| 311 | |
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| 312 | IF (firstcall) THEN |
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| 313 | |
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| 314 | write(*,*) 'Splitting radiative calculations: ', |
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| 315 | $ ' ngrid,ndomainsz,ndomain', |
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| 316 | $ ngrid,ndomainsz,ndomain |
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| 317 | |
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| 318 | c Assign a number to the different scatterers |
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| 319 | c ------------------------------------------- |
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| 320 | |
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| 321 | iaer_dust_conrath=0 |
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| 322 | iaer_dust_doubleq=0 |
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| 323 | iaer_dust_submicron=0 |
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| 324 | iaer_h2o_ice=0 |
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| 325 | iaer_co2_ice=0 |
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| 326 | iaer_stormdust_doubleq=0 |
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| 327 | iaer_topdust_doubleq=0 |
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| 328 | |
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| 329 | aer_count=0 |
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| 330 | if (.NOT.active) then |
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| 331 | do iaer=1,naerkind |
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| 332 | if (name_iaer(iaer).eq."dust_conrath") then |
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| 333 | iaer_dust_conrath = iaer |
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| 334 | aer_count = aer_count + 1 |
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| 335 | endif |
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| 336 | enddo |
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| 337 | endif |
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| 338 | if (doubleq.AND.active) then |
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| 339 | do iaer=1,naerkind |
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| 340 | if (name_iaer(iaer).eq."dust_doubleq") then |
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| 341 | iaer_dust_doubleq = iaer |
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| 342 | aer_count = aer_count + 1 |
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| 343 | endif |
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| 344 | enddo |
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| 345 | endif |
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| 346 | if (submicron.AND.active) then |
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| 347 | do iaer=1,naerkind |
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| 348 | if (name_iaer(iaer).eq."dust_submicron") then |
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| 349 | iaer_dust_submicron = iaer |
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| 350 | aer_count = aer_count + 1 |
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| 351 | endif |
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| 352 | enddo |
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| 353 | endif |
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| 354 | if (water.AND.activice) then |
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| 355 | do iaer=1,naerkind |
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| 356 | if (name_iaer(iaer).eq."h2o_ice") then |
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| 357 | iaer_h2o_ice = iaer |
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| 358 | aer_count = aer_count + 1 |
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| 359 | endif |
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| 360 | enddo |
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| 361 | endif |
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| 362 | if (co2clouds.AND.activeco2ice) then |
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| 363 | do iaer=1,naerkind |
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| 364 | if (name_iaer(iaer).eq."co2_ice") then |
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| 365 | iaer_co2_ice = iaer |
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| 366 | aer_count = aer_count + 1 |
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| 367 | endif |
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| 368 | enddo |
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| 369 | endif |
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| 370 | if (rdstorm.AND.active) then |
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| 371 | do iaer=1,naerkind |
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| 372 | if (name_iaer(iaer).eq."stormdust_doubleq") then |
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| 373 | iaer_stormdust_doubleq = iaer |
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| 374 | aer_count = aer_count + 1 |
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| 375 | endif |
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| 376 | enddo |
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| 377 | end if |
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| 378 | if (slpwind.AND.active) then |
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| 379 | do iaer=1,naerkind |
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| 380 | if (name_iaer(iaer).eq."topdust_doubleq") then |
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| 381 | iaer_topdust_doubleq = iaer |
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| 382 | aer_count = aer_count + 1 |
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| 383 | endif |
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| 384 | enddo |
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| 385 | end if |
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| 386 | |
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| 387 | c Check that we identified all tracers: |
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| 388 | if (aer_count.ne.naerkind) then |
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| 389 | write(*,*) "callradite: found only ",aer_count," scatterers" |
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| 390 | write(*,*) " expected ",naerkind |
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| 391 | write(*,*) "please make sure that the number of" |
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| 392 | write(*,*) "scatterers in scatterers.h, the names" |
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| 393 | write(*,*) "in callradite.F, and the flags in" |
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| 394 | write(*,*) "callphys.def are all consistent!" |
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| 395 | do iaer=1,naerkind |
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| 396 | write(*,*)' ',iaer,' ',trim(name_iaer(iaer)) |
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| 397 | enddo |
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| 398 | call abort_physic("callradite","incoherent scatterers",1) |
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| 399 | else |
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| 400 | write(*,*) "callradite: found all scatterers, namely:" |
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| 401 | do iaer=1,naerkind |
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| 402 | write(*,*)' ',iaer,' ',trim(name_iaer(iaer)) |
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| 403 | enddo |
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| 404 | endif |
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| 405 | c ------------------------------------------- |
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| 406 | |
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| 407 | gcp = g/cpp |
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| 408 | |
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| 409 | |
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| 410 | c Loading the optical properties in external look-up tables: |
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| 411 | |
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| 412 | CALL SUAER |
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| 413 | |
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| 414 | ! CALL SULW ! this step is now done in ini_yomlw_h |
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| 415 | |
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| 416 | if (ngrid .EQ. 1) then |
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| 417 | if (ndomainsz .NE. 1) then |
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| 418 | print* |
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| 419 | print*,'ATTENTION !!!' |
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| 420 | print*,'pour tourner en 1D, ' |
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| 421 | print*,'fixer ndomainsz=1 dans phymars/dimradmars_h' |
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| 422 | print* |
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| 423 | call exit(1) |
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| 424 | endif |
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| 425 | endif |
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| 426 | |
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| 427 | firstcall=.false. |
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| 428 | END IF |
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| 429 | |
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| 430 | c Computing aerosol optical properties and opacity |
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| 431 | c ------------------------------------------------ |
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| 432 | c Updating aerosol size distributions: |
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| 433 | CALL updatereffrad(ngrid,nlayer, |
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| 434 | & rdust,rstormdust,rtopdust,rice,nuice, |
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| 435 | & reffrad,nueffrad, riceco2, nuiceco2, |
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| 436 | & pq,tauscaling,tau,pplay, pt) |
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| 437 | c Computing 3D scattering parameters: |
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| 438 | gVIS3d(:,:,:,:) = 0. |
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| 439 | CALL aeroptproperties(ngrid,nlayer,reffrad,nueffrad, |
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| 440 | & QVISsQREF3d,omegaVIS3d,gVIS3d, |
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| 441 | & QIRsQREF3d,omegaIR3d,gIR3d, |
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| 442 | & QREFvis3d,QREFir3d, |
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| 443 | & omegaREFvis3d,omegaREFir3d) |
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| 444 | c Computing aerosol optical depth in each layer: |
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| 445 | CALL aeropacity(ngrid,nlayer,nq,zday,pplay,pplev,ls, |
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| 446 | & pq,pt,tauscaling,dust_rad_adjust,tau_pref_scenario, |
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| 447 | & tau_pref_gcm,tau,taucloudtes,aerosol,dsodust,reffrad, |
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| 448 | & QREFvis3d,QREFir3d,omegaREFir3d, |
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| 449 | & totstormfract,clearatm,dsords,dsotop, |
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| 450 | & alpha_hmons,nohmons, |
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| 451 | & clearsky,totcloudfrac) |
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| 452 | c Starting loop on sub-domain |
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| 453 | c ---------------------------- |
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| 454 | zgVIS3d(:,:,:,:) = 0. |
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| 455 | zfluxd_sw(:,:,:) = 0. |
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| 456 | zfluxu_sw(:,:,:) = 0. |
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| 457 | zQVISsQREF3d(:,:,:,:) = 0. |
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| 458 | zomegaVIS3d(:,:,:,:) = 0. |
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| 459 | DO jd=1,ndomain |
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| 460 | ig0=(jd-1)*ndomainsz |
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| 461 | if (jd.eq.ndomain) then |
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| 462 | nd=ngrid-ig0 |
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| 463 | else |
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| 464 | nd=ndomainsz |
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| 465 | endif |
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| 466 | |
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| 467 | c Spliting input variable in sub-domain input variables |
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| 468 | c --------------------------------------------------- |
|---|
| 469 | |
|---|
| 470 | do l=1,nlaylte |
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| 471 | do ig = 1,nd |
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| 472 | do iaer = 1, naerkind |
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| 473 | do ich = 1, nsun |
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| 474 | zQVISsQREF3d(ig,l,ich,iaer) = |
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| 475 | & QVISsQREF3d(ig0+ig,l,ich,iaer) |
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| 476 | zomegaVIS3d(ig,l,ich,iaer) = |
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| 477 | & omegaVIS3d(ig0+ig,l,ich,iaer) |
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| 478 | zgVIS3d(ig,l,ich,iaer) = |
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| 479 | & gVIS3d(ig0+ig,l,ich,iaer) |
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| 480 | enddo |
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| 481 | do ich = 1, nir |
|---|
| 482 | zQIRsQREF3d(ig,l,ich,iaer) = |
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| 483 | & QIRsQREF3d(ig0+ig,l,ich,iaer) |
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| 484 | zomegaIR3d(ig,l,ich,iaer) = |
|---|
| 485 | & omegaIR3d(ig0+ig,l,ich,iaer) |
|---|
| 486 | zgIR3d(ig,l,ich,iaer) = |
|---|
| 487 | & gIR3d(ig0+ig,l,ich,iaer) |
|---|
| 488 | enddo |
|---|
| 489 | enddo |
|---|
| 490 | enddo |
|---|
| 491 | enddo |
|---|
| 492 | zplev(:,:) = 0. |
|---|
| 493 | do l=1,nlaylte+1 |
|---|
| 494 | do ig = 1,nd |
|---|
| 495 | zplev(ig,l) = pplev(ig0+ig,l) |
|---|
| 496 | enddo |
|---|
| 497 | enddo |
|---|
| 498 | zdp(:,:) = 0. |
|---|
| 499 | |
|---|
| 500 | do l=1,nlaylte |
|---|
| 501 | do ig = 1,nd |
|---|
| 502 | zplay(ig,l) = pplay(ig0+ig,l) |
|---|
| 503 | zt(ig,l) = pt(ig0+ig,l) |
|---|
| 504 | c Thickness of each layer (Pa) : |
|---|
| 505 | zdp(ig,l)= pplev(ig0+ig,l) - pplev(ig0+ig,l+1) |
|---|
| 506 | enddo |
|---|
| 507 | enddo |
|---|
| 508 | zaerosol(:,:,:) = 0. |
|---|
| 509 | do n=1,naerkind |
|---|
| 510 | do l=1,nlaylte |
|---|
| 511 | do ig=1,nd |
|---|
| 512 | zaerosol(ig,l,n) = aerosol(ig0+ig,l,n) |
|---|
| 513 | enddo |
|---|
| 514 | enddo |
|---|
| 515 | enddo |
|---|
| 516 | zalbedo(:,:) = 0. |
|---|
| 517 | do j=1,2 |
|---|
| 518 | do ig = 1,nd |
|---|
| 519 | zalbedo(ig,j) = albedo(ig0+ig,j) |
|---|
| 520 | enddo |
|---|
| 521 | enddo |
|---|
| 522 | |
|---|
| 523 | c Intermediate levels: (computing tlev) |
|---|
| 524 | c --------------------------------------- |
|---|
| 525 | c Extrapolation for the air temperature above the surface |
|---|
| 526 | DO ig=1,nd |
|---|
| 527 | zztlev(ig,1)=zt(ig,1)+ |
|---|
| 528 | s (zplev(ig,1)-zplay(ig,1))* |
|---|
| 529 | s (zt(ig,1)-zt(ig,2))/(zplay(ig,1)-zplay(ig,2)) |
|---|
| 530 | |
|---|
| 531 | zdt0(ig) = tsurf(ig0+ig) - zztlev(ig,1) |
|---|
| 532 | ENDDO |
|---|
| 533 | |
|---|
| 534 | DO l=2,nlaylte |
|---|
| 535 | DO ig=1, nd |
|---|
| 536 | zztlev(ig,l)=0.5*(zt(ig,l-1)+zt(ig,l)) |
|---|
| 537 | ENDDO |
|---|
| 538 | ENDDO |
|---|
| 539 | |
|---|
| 540 | DO ig=1, nd |
|---|
| 541 | zztlev(ig,nlaylte+1)=zt(ig,nlaylte) |
|---|
| 542 | ENDDO |
|---|
| 543 | |
|---|
| 544 | |
|---|
| 545 | c Longwave ("lw") radiative transfer (= thermal infrared) |
|---|
| 546 | c ------------------------------------------------------- |
|---|
| 547 | call lwmain (ig0,icount,nd,nflev |
|---|
| 548 | . ,zdp,zdt0,emis(ig0+1),zplev,zztlev,zt |
|---|
| 549 | . ,zaerosol,zzdtlw |
|---|
| 550 | . ,fluxsurf_lw(ig0+1),fluxtop_lw(ig0+1) |
|---|
| 551 | . ,znetrad |
|---|
| 552 | & ,zQIRsQREF3d,zomegaIR3d,zgIR3d |
|---|
| 553 | & ,co2ice(ig0+1)) |
|---|
| 554 | |
|---|
| 555 | c Shortwave ("sw") radiative transfer (= solar radiation) |
|---|
| 556 | c ------------------------------------------------------- |
|---|
| 557 | c Mars solar constant (W m-2) |
|---|
| 558 | c 1370 W.m-2 is the solar constant at 1 AU. |
|---|
| 559 | cste_mars=1370./(dist_sol*dist_sol) |
|---|
| 560 | zzdtsw(:,:) = 0. |
|---|
| 561 | call swmain ( nd, nflev, |
|---|
| 562 | S cste_mars, zalbedo, |
|---|
| 563 | S mu0(ig0+1), zdp, zplev, zaerosol, fract(ig0+1), |
|---|
| 564 | S zzdtsw, zfluxd_sw, zfluxu_sw, |
|---|
| 565 | & zQVISsQREF3d,zomegaVIS3d,zgVIS3d) |
|---|
| 566 | c ------------------------------------------------------------ |
|---|
| 567 | c Un-spliting output variable from sub-domain input variables |
|---|
| 568 | c ------------------------------------------------------------ |
|---|
| 569 | |
|---|
| 570 | do l=1,nlaylte |
|---|
| 571 | do ig = 1,nd |
|---|
| 572 | dtlw(ig0+ig,l) = zzdtlw(ig,l) |
|---|
| 573 | dtsw(ig0+ig,l) = zzdtsw(ig,l) |
|---|
| 574 | enddo |
|---|
| 575 | enddo |
|---|
| 576 | |
|---|
| 577 | ptlev(:, :) = 0. |
|---|
| 578 | do l=1,nlaylte+1 |
|---|
| 579 | do ig = 1,nd |
|---|
| 580 | ptlev(ig0+ig,l) = zztlev(ig,l) |
|---|
| 581 | enddo |
|---|
| 582 | enddo |
|---|
| 583 | |
|---|
| 584 | do ig = 1,nd |
|---|
| 585 | fluxsurf_sw(ig0+ig,1) = zfluxd_sw(ig,1,1) |
|---|
| 586 | fluxsurf_sw(ig0+ig,2) = zfluxd_sw(ig,1,2) |
|---|
| 587 | fluxtop_sw(ig0+ig,1) = zfluxu_sw(ig,nlaylte+1,1) |
|---|
| 588 | fluxtop_sw(ig0+ig,2) = zfluxu_sw(ig,nlaylte+1,2) |
|---|
| 589 | enddo |
|---|
| 590 | |
|---|
| 591 | ENDDO ! (boucle jd=1, ndomain) |
|---|
| 592 | |
|---|
| 593 | c Zero tendencies for any remaining layers between nlaylte and nlayer |
|---|
| 594 | if (nlayer.gt.nlaylte) then |
|---|
| 595 | do l = nlaylte+1, nlayer |
|---|
| 596 | do ig = 1, ngrid |
|---|
| 597 | dtlw(ig, l) = 0. |
|---|
| 598 | dtsw(ig, l) = 0. |
|---|
| 599 | enddo |
|---|
| 600 | enddo |
|---|
| 601 | endif |
|---|
| 602 | c Output for debugging if lwrite=T |
|---|
| 603 | c -------------------------------- |
|---|
| 604 | c Write all nlayer layers, even though only nlaylte layers may have |
|---|
| 605 | c non-zero tendencies. |
|---|
| 606 | |
|---|
| 607 | IF(lwrite) THEN |
|---|
| 608 | PRINT*,'Diagnotique for the radiation' |
|---|
| 609 | PRINT*,'albedo, emissiv, mu0,fract,fluxsurf_lw,fluxsurf_sw' |
|---|
| 610 | PRINT*,albedo(igout,1),emis(igout),mu0(igout), |
|---|
| 611 | s fract(igout), fluxsurf_lw(igout), |
|---|
| 612 | $ fluxsurf_sw(igout,1)+fluxsurf_sw(igout,2) |
|---|
| 613 | PRINT*,'Tlay Tlev Play Plev dT/dt SW dT/dt LW (K/s)' |
|---|
| 614 | PRINT*,'daysec',daysec |
|---|
| 615 | DO l=1,nlayer |
|---|
| 616 | PRINT*,pt(igout,l),ptlev(igout,l), |
|---|
| 617 | s pplay(igout,l),pplev(igout,l), |
|---|
| 618 | s dtsw(igout,l),dtlw(igout,l) |
|---|
| 619 | ENDDO |
|---|
| 620 | ENDIF |
|---|
| 621 | |
|---|
| 622 | |
|---|
| 623 | END SUBROUTINE callradite |
|---|
| 624 | |
|---|
| 625 | END MODULE callradite_mod |
|---|
