| 1 | SUBROUTINE co2cloud(ngrid,nlay,ptimestep, |
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| 2 | & pplev,pplay,pdpsrf,pzlay,pt,pdt, |
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| 3 | & pq,pdq,pdqcloudco2,pdtcloudco2, |
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| 4 | & nq,tau,tauscaling,rdust,rice,riceco2,nuice, |
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| 5 | & rsedcloudco2,rhocloudco2, |
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| 6 | & rsedcloud,rhocloud,pzlev,pdqs_sedco2, |
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| 7 | & pdu,pu) |
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| 8 | ! to use 'getin' |
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| 9 | use dimradmars_mod, only: naerkind |
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| 10 | USE comcstfi_h |
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| 11 | USE ioipsl_getincom |
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| 12 | USE updaterad |
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| 13 | use conc_mod, only: mmean,rnew |
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| 14 | use tracer_mod, only: nqmx, igcm_co2, igcm_co2_ice, |
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| 15 | & igcm_dust_mass, igcm_dust_number,igcm_h2o_ice, |
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| 16 | & igcm_ccn_mass,igcm_ccn_number, |
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| 17 | & igcm_ccnco2_mass, igcm_ccnco2_number, |
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| 18 | & rho_dust, nuiceco2_sed, nuiceco2_ref, |
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| 19 | & rho_ice_co2,r3n_q,rho_ice,nuice_sed |
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| 20 | |
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| 21 | IMPLICIT NONE |
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| 22 | |
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| 23 | #include "datafile.h" |
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| 24 | #include "callkeys.h" |
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| 25 | #include "microphys.h" |
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| 26 | |
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| 27 | c======================================================================= |
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| 28 | c CO2 clouds formation |
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| 29 | c |
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| 30 | c There is a time loop specific to cloud formation |
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| 31 | c due to timescales smaller than the GCM integration timestep. |
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| 32 | c microphysics subroutine is improvedCO2clouds.F |
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| 33 | c the microphysics time step is a fraction of the physical one |
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| 34 | c the integer imicroco2 must be set in callphys.def |
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| 35 | c |
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| 36 | c The co2 clouds tracers (co2_ice, ccn mass and concentration) are |
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| 37 | c sedimented at each microtimestep. pdqs_sedco2 keeps track of the |
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| 38 | c CO2 flux at the surface |
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| 39 | c |
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| 40 | c Authors: 09/2016 Joachim Audouard & Constantino Listowski |
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| 41 | c Adaptation of the water ice clouds scheme (with specific microphysics) |
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| 42 | c of Montmessin, Navarro & al. |
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| 43 | c |
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| 44 | c 07/2017 J.Audouard |
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| 45 | c Several logicals and integer must be set to .true. in callphys.def |
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| 46 | c uf not, default values are .false. |
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| 47 | c co2clouds=.true. call this routine |
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| 48 | c co2useh2o=.true. allow the use of water ice particles as CCN for CO2 |
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| 49 | c meteo_flux=.true. supply meteoritic particles |
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| 50 | c CLFvaryingCO2=.true. allows a subgrid temperature distribution |
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| 51 | c of amplitude spantCO2(=integer in callphys.def) |
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| 52 | c imicroco2=50 |
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| 53 | c |
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| 54 | c The subgrid Temperature distribution is modulated (0 or 1) by Spiga et |
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| 55 | c al. (GRL 2012) Saturation Index to account for GW propagation or |
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| 56 | c dissipation upwards. |
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| 57 | c |
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| 58 | c 4D and column opacities are computed using Qext values at 1µm. |
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| 59 | c======================================================================= |
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| 60 | |
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| 61 | c----------------------------------------------------------------------- |
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| 62 | c declarations: |
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| 63 | c ------------- |
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| 64 | |
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| 65 | c Inputs: |
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| 66 | c ------ |
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| 67 | |
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| 68 | INTEGER ngrid,nlay |
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| 69 | INTEGER nq ! nombre de traceurs |
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| 70 | REAL ptimestep ! pas de temps physique (s) |
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| 71 | REAL pplev(ngrid,nlay+1) ! pression aux inter-couches (Pa) |
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| 72 | REAL pplay(ngrid,nlay) ! pression au milieu des couches (Pa) |
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| 73 | REAL pdpsrf(ngrid) ! tendence surf pressure |
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| 74 | REAL pzlay(ngrid,nlay) ! altitude at the middle of the layers |
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| 75 | REAL pt(ngrid,nlay) ! temperature at the middle of the layers (K) |
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| 76 | REAL pdt(ngrid,nlay) ! tendence temperature des autres param. |
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| 77 | real,intent(in) :: pzlev(ngrid,nlay+1) ! altitude at the boundaries of the layers |
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| 78 | real pq(ngrid,nlay,nq) ! traceur (kg/kg) |
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| 79 | real pdq(ngrid,nlay,nq) ! tendance avant condensation (kg/kg.s-1) |
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| 80 | |
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| 81 | real rice(ngrid,nlay) ! Water Ice mass mean radius (m) |
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| 82 | ! used for nucleation of CO2 on ice-coated ccns |
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| 83 | DOUBLE PRECISION rho_ice_co2T(ngrid,nlay) !T-dependant CO2 ice density |
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| 84 | DOUBLE PRECISION :: myT ! temperature scalar for co2 density computation |
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| 85 | REAL tau(ngrid,naerkind) ! Column dust optical depth at each point |
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| 86 | REAL tauscaling(ngrid) ! Convertion factor for dust amount |
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| 87 | real rdust(ngrid,nlay) ! Dust geometric mean radius (m) |
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| 88 | |
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| 89 | c Outputs: |
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| 90 | c ------- |
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| 91 | |
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| 92 | real pdqcloudco2(ngrid,nlay,nq) ! tendence de la condensation H2O(kg/kg.s-1) |
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| 93 | REAL pdtcloudco2(ngrid,nlay) ! tendence temperature due |
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| 94 | ! a la chaleur latente |
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| 95 | DOUBLE PRECISION riceco2(ngrid,nlay) ! Ice mass mean radius (m) |
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| 96 | ! (r_c in montmessin_2004) |
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| 97 | REAL nuice(ngrid,nlay) ! Estimated effective variance |
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| 98 | ! of the size distribution |
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| 99 | real rsedcloudco2(ngrid,nlay) ! Cloud sedimentation radius |
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| 100 | real rhocloudco2(ngrid,nlay) ! Cloud density (kg.m-3) |
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| 101 | real rhocloudco2t(ngrid,nlay) ! Cloud density (kg.m-3) |
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| 102 | real pdqs_sedco2(ngrid) ! CO2 flux at the surface |
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| 103 | |
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| 104 | c local: |
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| 105 | c ------ |
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| 106 | !water |
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| 107 | real rsedcloud(ngrid,nlay) ! Cloud sedimentation radius |
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| 108 | real rhocloud(ngrid,nlay) ! Cloud density (kg.m-3) |
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| 109 | ! for ice radius computation |
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| 110 | |
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| 111 | ! for time loop |
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| 112 | INTEGER microstep ! time subsampling step variable |
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| 113 | INTEGER imicroco2 ! time subsampling for coupled water microphysics & sedimentation |
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| 114 | SAVE imicroco2 |
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| 115 | REAL microtimestep ! integration timestep for coupled water microphysics & sedimentation |
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| 116 | SAVE microtimestep |
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| 117 | |
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| 118 | ! tendency given by clouds (inside the micro loop) |
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| 119 | REAL subpdqcloudco2(ngrid,nlay,nq) ! cf. pdqcloud |
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| 120 | REAL subpdtcloudco2(ngrid,nlay) ! cf. pdtcloud |
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| 121 | |
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| 122 | ! global tendency (clouds+physics) |
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| 123 | REAL subpdq(ngrid,nlay,nq) ! cf. pdqcloud |
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| 124 | REAL subpdt(ngrid,nlay) ! cf. pdtcloud |
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| 125 | real wq(ngrid,nlay+1) ! ! displaced tracer mass (kg.m-2) during microtimestep because sedim (?/m-2) |
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| 126 | |
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| 127 | REAL satuco2(ngrid,nlay) ! co2 satu ratio for output |
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| 128 | REAL zqsatco2(ngrid,nlay) ! saturation co2 |
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| 129 | |
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| 130 | INTEGER iq,ig,l,i |
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| 131 | LOGICAL,SAVE :: firstcall=.true. |
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| 132 | DOUBLE PRECISION Nccnco2, Niceco2,Nco2,Qccnco2 |
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| 133 | real :: beta ! for sedimentation |
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| 134 | |
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| 135 | real epaisseur (ngrid,nlay) ! Layer thickness (m) |
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| 136 | real masse (ngrid,nlay) ! Layer mass (kg.m-2) |
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| 137 | real tempo_traceur_t(ngrid,nlay) ! tracers with real-time value in microtimeloop |
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| 138 | real tempo_traceurs(ngrid,nlay,nq) |
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| 139 | real sav_trac(ngrid,nlay,nq) !For sedimentation tendancy |
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| 140 | real pdqsed(ngrid,nlay,nq) |
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| 141 | |
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| 142 | DOUBLE PRECISION,allocatable,save :: memdMMccn(:,:) !memory of h2o particles |
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| 143 | DOUBLE PRECISION,allocatable,save :: memdMMh2o(:,:) !only if co2useh2o=.true. |
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| 144 | DOUBLE PRECISION,allocatable,save :: memdNNccn(:,:) !Nb particules H2O intégré |
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| 145 | |
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| 146 | ! What we need for Qext reading and tau computation : size distribution |
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| 147 | DOUBLE PRECISION vrat_cld ! Volume ratio |
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| 148 | DOUBLE PRECISION rb_cldco2(nbinco2_cld+1) ! boundary values of each rad_cldco2 bin (m) |
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| 149 | SAVE rb_cldco2 |
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| 150 | DOUBLE PRECISION, PARAMETER :: rmin_cld = 1.e-9 ! Minimum radius (m) |
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| 151 | DOUBLE PRECISION, PARAMETER :: rmax_cld = 5.e-6 ! Maximum radius (m) |
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| 152 | DOUBLE PRECISION, PARAMETER :: rbmin_cld =1.e-10! Minimum boundary radius (m) |
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| 153 | DOUBLE PRECISION, PARAMETER :: rbmax_cld = 2.e-4 ! Maximum boundary radius (m) |
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| 154 | DOUBLE PRECISION dr_cld(nbinco2_cld) ! width of each rad_cldco2 bin (m) |
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| 155 | DOUBLE PRECISION vol_cld(nbinco2_cld) ! particle volume for each bin (m3) |
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| 156 | REAL sigma_iceco2 ! Variance of the ice and CCN distributions |
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| 157 | logical :: file_ok !Qext file reading |
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| 158 | double precision :: radv(10000),Qextv1mic(10000) |
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| 159 | double precision :: Qext1bins(100),Qtemp |
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| 160 | double precision :: ltemp1(10000),ltemp2(10000) |
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| 161 | integer :: nelem,lebon1,lebon2,uQext |
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| 162 | save Qext1bins |
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| 163 | DOUBLE PRECISION n_aer(nbinco2_cld),Rn,No,n_derf,dev2 |
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| 164 | DOUBLE PRECISION Qext1bins2(ngrid,nlay) |
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| 165 | DOUBLE PRECISION tau1mic(ngrid) !co2 ice column opacity at 1µm |
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| 166 | |
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| 167 | ! For sub grid T distribution |
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| 168 | |
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| 169 | REAL zt(ngrid,nlay) ! local value of temperature |
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| 170 | REAL :: zq(ngrid, nlay,nq) |
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| 171 | |
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| 172 | DOUBLE PRECISION :: tcond(ngrid,nlay) !CO2 condensation temperature |
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| 173 | REAL :: zqvap(ngrid,nlay) |
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| 174 | REAL :: zqice(ngrid,nlay) |
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| 175 | REAL :: spant,zdelt ! delta T for the temperature distribution |
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| 176 | REAL :: zteff(ngrid, nlay)! effective temperature in the cloud,neb |
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| 177 | REAL :: pqeff(ngrid, nlay, nq)! effective tracers quantities in the cloud |
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| 178 | REAL :: cloudfrac(ngrid,nlay) ! cloud fraction |
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| 179 | REAL :: mincloud ! min cloud frac |
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| 180 | DOUBLE PRECISION:: rho,zu,NN,gradT !For Saturation Index computation |
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| 181 | REAL :: pdu(ngrid,nlay),pu(ngrid,nlay) !Wind field zu=pu+pdu*ptimestep |
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| 182 | DOUBLE PRECISION :: SatIndex(ngrid,nlay),SatIndexmap(ngrid) |
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| 183 | |
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| 184 | c logical :: CLFvaryingCO2 |
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| 185 | c ** un petit test de coherence |
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| 186 | c -------------------------- |
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| 187 | |
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| 188 | IF (firstcall) THEN |
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| 189 | if (nq.gt.nqmx) then |
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| 190 | write(*,*) 'stop in co2cloud (nq.gt.nqmx)!' |
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| 191 | write(*,*) 'nq=',nq,' nqmx=',nqmx |
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| 192 | stop |
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| 193 | endif |
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| 194 | write(*,*) "co2cloud.F: rho_ice_co2 = ",rho_ice_co2 |
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| 195 | write(*,*) "co2cloud: igcm_co2=",igcm_co2 |
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| 196 | write(*,*) " igcm_co2_ice=",igcm_co2_ice |
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| 197 | |
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| 198 | write(*,*) "time subsampling for microphysic ?" |
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| 199 | #ifdef MESOSCALE |
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| 200 | imicroco2 = 2 |
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| 201 | #else |
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| 202 | imicroco2 = 30 |
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| 203 | #endif |
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| 204 | call getin("imicroco2",imicroco2) |
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| 205 | write(*,*)"imicroco2 = ",imicroco2 |
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| 206 | |
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| 207 | microtimestep = ptimestep/real(imicroco2) |
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| 208 | write(*,*)"Physical timestep is",ptimestep |
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| 209 | write(*,*)"CO2 Microphysics timestep is",microtimestep |
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| 210 | |
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| 211 | |
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| 212 | if (.not. allocated(memdMMccn)) allocate(memdMMccn(ngrid,nlay)) |
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| 213 | if (.not. allocated(memdNNccn)) allocate(memdNNccn(ngrid,nlay)) |
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| 214 | if (.not. allocated(memdMMh2o)) allocate(memdMMh2o(ngrid,nlay)) |
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| 215 | |
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| 216 | memdMMccn(:,:)=0. |
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| 217 | memdMMh2o(:,:)=0. |
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| 218 | memdNNccn(:,:)=0. |
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| 219 | |
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| 220 | c Compute the size bins of the distribution of CO2 ice particles |
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| 221 | c --> used for opacity calculations |
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| 222 | |
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| 223 | c rad_cldco2 is the primary radius grid used for microphysics computation. |
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| 224 | c The grid spacing is computed assuming a constant volume ratio |
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| 225 | c between two consecutive bins; i.e. vrat_cld. |
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| 226 | c vrat_cld is determined from the boundary values of the size grid: |
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| 227 | c rmin_cld and rmax_cld. |
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| 228 | c The rb_cldco2 array contains the boundary values of each rad_cldco2 bin. |
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| 229 | c dr_cld is the width of each rad_cldco2 bin. |
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| 230 | sigma_iceco2 = sqrt(log(1.+nuiceco2_sed)) |
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| 231 | c Volume ratio between two adjacent bins |
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| 232 | ! vrat_cld |
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| 233 | vrat_cld = log(rmax_cld/rmin_cld) / float(nbinco2_cld-1) *3. |
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| 234 | vrat_cld = exp(vrat_cld) |
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| 235 | rb_cldco2(1) = rbmin_cld |
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| 236 | rad_cldco2(1) = rmin_cld |
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| 237 | vol_cld(1) = 4./3. * dble(pi) * rmin_cld*rmin_cld*rmin_cld |
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| 238 | do i=1,nbinco2_cld-1 |
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| 239 | rad_cldco2(i+1) = rad_cldco2(i) * vrat_cld**(1./3.) |
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| 240 | vol_cld(i+1) = vol_cld(i) * vrat_cld |
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| 241 | enddo |
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| 242 | do i=1,nbinco2_cld |
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| 243 | rb_cldco2(i+1)= ( (2.*vrat_cld) / (vrat_cld+1.) )**(1./3.) * |
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| 244 | & rad_cldco2(i) |
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| 245 | dr_cld(i) = rb_cldco2(i+1) - rb_cldco2(i) |
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| 246 | enddo |
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| 247 | rb_cldco2(nbinco2_cld+1) = rbmax_cld |
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| 248 | dr_cld(nbinco2_cld) = rb_cldco2(nbinco2_cld+1) - |
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| 249 | & rb_cldco2(nbinco2_cld) |
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| 250 | |
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| 251 | c read the Qext values |
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| 252 | INQUIRE(FILE=datafile(1:LEN_TRIM(datafile))// |
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| 253 | & '/optprop_co2ice_1mic.dat', EXIST=file_ok) |
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| 254 | IF (.not. file_ok) THEN |
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| 255 | write(*,*) 'file optprop_co2ice_1mic.dat should be in ' |
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| 256 | & ,datafile |
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| 257 | STOP |
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| 258 | endif |
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| 259 | open(newunit=uQext,file=trim(datafile)// |
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| 260 | & '/optprop_co2ice_1mic.dat' |
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| 261 | & ,FORM='formatted') |
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| 262 | read(uQext,*) !skip 1 line |
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| 263 | do i=1,10000 |
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| 264 | read(uQext,'(E11.5)') radv(i) |
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| 265 | enddo |
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| 266 | read(uQext,*) !skip 1 line |
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| 267 | do i=1,10000 |
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| 268 | read(uQext,'(E11.5)') Qextv1mic(i) |
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| 269 | enddo |
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| 270 | close(uQext) |
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| 271 | c innterpol the Qext values |
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| 272 | !rice_out=rad_cldco2 |
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| 273 | do i=1,nbinco2_cld |
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| 274 | ltemp1=abs(radv(:)-rb_cldco2(i)) |
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| 275 | ltemp2=abs(radv(:)-rb_cldco2(i+1)) |
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| 276 | lebon1=minloc(ltemp1,DIM=1) |
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| 277 | lebon2=min(minloc(ltemp2,DIM=1),10000) |
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| 278 | nelem=lebon2-lebon1+1. |
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| 279 | Qtemp=0d0 |
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| 280 | do l=0,nelem |
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| 281 | Qtemp=Qtemp+Qextv1mic(min(lebon1+l,10000)) !mean value in the interval |
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| 282 | enddo |
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| 283 | Qtemp=Qtemp/nelem |
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| 284 | Qext1bins(i)=Qtemp |
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| 285 | enddo |
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| 286 | Qext1bins(:)=Qext1bins(:)*rad_cldco2(:)*rad_cldco2(:)*pi |
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| 287 | ! The actuall tau computation and output is performed in co2cloud.F |
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| 288 | |
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| 289 | print*,'--------------------------------------------' |
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| 290 | print*,'Microphysics co2: size bin-Qext information:' |
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| 291 | print*,' i, rad_cldco2(i), Qext1bins(i)' |
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| 292 | do i=1,nbinco2_cld |
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| 293 | write(*,'(i3,3x,3(e12.6,4x))') i, rad_cldco2(i), |
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| 294 | & Qext1bins(i) |
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| 295 | enddo |
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| 296 | print*,'--------------------------------------------' |
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| 297 | |
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| 298 | |
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| 299 | do i=1,nbinco2_cld+1 |
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| 300 | rb_cldco2(i) = log(rb_cldco2(i)) !! we save that so that it is not computed at each timestep and gridpoint |
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| 301 | enddo |
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| 302 | if (CLFvaryingCO2) then |
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| 303 | write(*,*) |
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| 304 | write(*,*) "CLFvaryingCO2 is set to true is callphys.def" |
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| 305 | write(*,*) "The temperature field is enlarged to +/-",spantCO2 |
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| 306 | write(*,*) "for the CO2 microphysics " |
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| 307 | endif |
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| 308 | |
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| 309 | firstcall=.false. |
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| 310 | ENDIF ! of IF (firstcall) |
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| 311 | |
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| 312 | c-----Initialization |
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| 313 | dev2 = 1. / ( sqrt(2.) * sigma_iceco2 ) |
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| 314 | beta=0.85 |
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| 315 | subpdq(1:ngrid,1:nlay,1:nq) = 0 |
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| 316 | subpdt(1:ngrid,1:nlay) = 0 |
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| 317 | subpdqcloudco2(1:ngrid,1:nlay,1:nq) = 0 |
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| 318 | subpdtcloudco2(1:ngrid,1:nlay) = 0 |
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| 319 | |
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| 320 | wq(:,:)=0 |
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| 321 | ! default value if no ice |
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| 322 | rhocloudco2(1:ngrid,1:nlay) = rho_dust |
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| 323 | rhocloudco2t(1:ngrid,1:nlay) = rho_dust |
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| 324 | epaisseur(1:ngrid,1:nlay)=0 |
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| 325 | masse(1:ngrid,1:nlay)=0 |
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| 326 | |
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| 327 | sav_trac(1:ngrid,1:nlay,1:nq)=0 |
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| 328 | pdqsed(1:ngrid,1:nlay,1:nq)=0 |
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| 329 | |
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| 330 | do l=1,nlay |
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| 331 | do ig=1, ngrid |
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| 332 | masse(ig,l)=(pplev(ig,l) - pplev(ig,l+1)) /g |
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| 333 | epaisseur(ig,l)= pzlev(ig,l+1) - pzlev(ig,l) |
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| 334 | enddo |
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| 335 | enddo |
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| 336 | |
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| 337 | c------------------------------------------------------------------- |
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| 338 | c 0. Representation of sub-grid water ice clouds |
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| 339 | c------------------------------------------------------------------- |
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| 340 | IF (CLFvaryingCO2) THEN |
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| 341 | |
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| 342 | spant=spantCO2 ! delta T for the temprature distribution |
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| 343 | mincloud=0.1 ! min cloudfrac when there is ice |
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| 344 | zteff(:,:)=pt(:,:) |
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| 345 | cloudfrac(:,:)=mincloud |
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| 346 | |
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| 347 | c-----Tendencies |
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| 348 | DO l=1,nlay |
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| 349 | DO ig=1,ngrid |
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| 350 | zt(ig,l)=pt(ig,l)+ pdt(ig,l)*ptimestep |
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| 351 | ENDDO |
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| 352 | ENDDO |
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| 353 | DO l=1,nlay |
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| 354 | DO ig=1,ngrid |
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| 355 | DO iq=1,nq |
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| 356 | zq(ig,l,iq)=pq(ig,l,iq)+pdq(ig,l,iq)*ptimestep |
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| 357 | ENDDO |
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| 358 | ENDDO |
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| 359 | ENDDO |
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| 360 | zqvap=zq(:,:,igcm_co2) |
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| 361 | zqice=zq(:,:,igcm_co2_ice) |
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| 362 | |
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| 363 | |
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| 364 | call WRITEDIAGFI(ngrid,"pzlev","pzlev","km",3, |
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| 365 | & pzlev) |
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| 366 | call WRITEDIAGFI(ngrid,"pzlay","pzlay","km",3, |
|---|
| 367 | & pzlay) |
|---|
| 368 | call WRITEDIAGFI(ngrid,"pplay","pplay","Pa",3, |
|---|
| 369 | & pplay) |
|---|
| 370 | |
|---|
| 371 | DO l=12,26 |
|---|
| 372 | ! layers 12 --> 26 ~ 12->85 km |
|---|
| 373 | DO ig=1,ngrid |
|---|
| 374 | ! Calcul de N^2 static stability |
|---|
| 375 | gradT=(zt(ig,l+1)-zt(ig,l))/(pzlev(ig,l+1)-pzlev(ig,l)) |
|---|
| 376 | NN=sqrt(g/zt(iq,l)*(max(gradT,-g/cpp)+g/cpp)) |
|---|
| 377 | !calcul of wind field |
|---|
| 378 | zu=pu(ig,l) + pdu(ig,l)*ptimestep |
|---|
| 379 | ! calcul of background density |
|---|
| 380 | rho=pplay(ig,l)/(rnew(ig,l)*zt(ig,l)) |
|---|
| 381 | !saturation index |
|---|
| 382 | SatIndex(ig,l)=sqrt(7.5e-7*150.e3/(2.*pi)*NN/(rho*zu*zu*zu)) |
|---|
| 383 | enddo |
|---|
| 384 | enddo |
|---|
| 385 | !Then compute Satindex map |
|---|
| 386 | ! layers 12 --> 26 ~ 12->85 km |
|---|
| 387 | DO ig=1,ngrid |
|---|
| 388 | SatIndexmap(ig)=maxval(SatIndex(ig,12:26)) |
|---|
| 389 | enddo |
|---|
| 390 | |
|---|
| 391 | call WRITEDIAGFI(ngrid,"SatIndexmap","SatIndexmap","km",2, |
|---|
| 392 | & SatIndexmap) |
|---|
| 393 | |
|---|
| 394 | !Modulate the DeltaT by GW propagation index : |
|---|
| 395 | ! Saturation index S in Spiga 2012 paper |
|---|
| 396 | !Assuming like in the paper, |
|---|
| 397 | !GW phase speed (stationary waves) c=0 m.s-1 |
|---|
| 398 | !lambdaH =150 km |
|---|
| 399 | !Fo=7.5e-7 J.m-3 |
|---|
| 400 | |
|---|
| 401 | CALL tcondco2(ngrid,nlay,pplay,zqvap,tcond) |
|---|
| 402 | ! A tester: CALL tcondco2(ngrid,nlay,pplay,zqvap,tcond) |
|---|
| 403 | zdelt=spant |
|---|
| 404 | DO ig=1,ngrid |
|---|
| 405 | |
|---|
| 406 | if (SatIndexmap(ig) .le. 0.1) THEN |
|---|
| 407 | DO l=1,nlay-1 |
|---|
| 408 | |
|---|
| 409 | IF (tcond(ig,l) .ge. (zt(ig,l)+zdelt) |
|---|
| 410 | & .or. tcond(ig,l) .le. 0 ) THEN !Toute la fraction est saturée |
|---|
| 411 | zteff(ig,l)=zt(ig,l) |
|---|
| 412 | cloudfrac(ig,l)=1. |
|---|
| 413 | ELSE IF (tcond(ig,l) .le. (zt(ig,l)-zdelt)) THEN !Rien n'est saturé |
|---|
| 414 | zteff(ig,l)=zt(ig,l)-zdelt |
|---|
| 415 | cloudfrac(ig,l)=mincloud |
|---|
| 416 | ELSE |
|---|
| 417 | cloudfrac(ig,l)=(tcond(ig,l)-zt(ig,l)+zdelt)/ |
|---|
| 418 | & (2.0*zdelt) |
|---|
| 419 | zteff(ig,l)=(tcond(ig,l)+zt(ig,l)-zdelt)/2. !Temperature moyenne de la fraction nuageuse |
|---|
| 420 | END IF !ig if (tcond(ig,l) ... |
|---|
| 421 | zteff(ig,l)=zteff(ig,l)-pdt(ig,l)*ptimestep |
|---|
| 422 | IF (cloudfrac(ig,l).le. mincloud) THEN |
|---|
| 423 | cloudfrac(ig,l)=mincloud |
|---|
| 424 | ELSE IF (cloudfrac(ig,l).gt. 1) THEN |
|---|
| 425 | cloudfrac(ig,l)=1. |
|---|
| 426 | END IF |
|---|
| 427 | ENDDO |
|---|
| 428 | ELSE |
|---|
| 429 | !SatIndex not favorable for GW : leave pt untouched |
|---|
| 430 | zteff(ig,l)=pt(ig,l) |
|---|
| 431 | cloudfrac(ig,l)=mincloud |
|---|
| 432 | END IF ! of if(SatIndexmap... |
|---|
| 433 | ENDDO |
|---|
| 434 | ! Totalcloud frac of the column missing here |
|---|
| 435 | c----------------------- |
|---|
| 436 | c-----No sub-grid cloud representation (CLFvarying=false) |
|---|
| 437 | ELSE |
|---|
| 438 | DO l=1,nlay |
|---|
| 439 | DO ig=1,ngrid |
|---|
| 440 | zteff(ig,l)=pt(ig,l) |
|---|
| 441 | END DO |
|---|
| 442 | END DO |
|---|
| 443 | END IF ! end if (CLFvaryingco2) |
|---|
| 444 | c------------------------------------------------------------------ |
|---|
| 445 | c microtimestep timeloop for microphysics: |
|---|
| 446 | c 0.Stepped entry for tendancies |
|---|
| 447 | c 1.Compute sedimentation and update tendancies |
|---|
| 448 | c 2.Call co2clouds microphysics |
|---|
| 449 | c 3.Update tendancies |
|---|
| 450 | c------------------------------------------------------------------ |
|---|
| 451 | DO microstep=1,imicroco2 |
|---|
| 452 | c------ Temperature tendency subpdt |
|---|
| 453 | ! If imicro=1 subpdt is the same as pdt |
|---|
| 454 | DO l=1,nlay |
|---|
| 455 | DO ig=1,ngrid |
|---|
| 456 | subpdt(ig,l) = subpdt(ig,l) |
|---|
| 457 | & + pdt(ig,l) ! At each micro timestep we add pdt in order to have a stepped entry |
|---|
| 458 | subpdq(ig,l,igcm_dust_mass) = |
|---|
| 459 | & subpdq(ig,l,igcm_dust_mass) |
|---|
| 460 | & + pdq(ig,l,igcm_dust_mass) |
|---|
| 461 | subpdq(ig,l,igcm_dust_number) = |
|---|
| 462 | & subpdq(ig,l,igcm_dust_number) |
|---|
| 463 | & + pdq(ig,l,igcm_dust_number) |
|---|
| 464 | |
|---|
| 465 | subpdq(ig,l,igcm_ccnco2_mass) = |
|---|
| 466 | & subpdq(ig,l,igcm_ccnco2_mass) |
|---|
| 467 | & + pdq(ig,l,igcm_ccnco2_mass) |
|---|
| 468 | subpdq(ig,l,igcm_ccnco2_number) = |
|---|
| 469 | & subpdq(ig,l,igcm_ccnco2_number) |
|---|
| 470 | & + pdq(ig,l,igcm_ccnco2_number) |
|---|
| 471 | |
|---|
| 472 | subpdq(ig,l,igcm_co2_ice) = |
|---|
| 473 | & subpdq(ig,l,igcm_co2_ice) |
|---|
| 474 | & + pdq(ig,l,igcm_co2_ice) |
|---|
| 475 | subpdq(ig,l,igcm_co2) = |
|---|
| 476 | & subpdq(ig,l,igcm_co2) |
|---|
| 477 | & + pdq(ig,l,igcm_co2) |
|---|
| 478 | |
|---|
| 479 | subpdq(ig,l,igcm_h2o_ice) = |
|---|
| 480 | & subpdq(ig,l,igcm_h2o_ice) |
|---|
| 481 | & + pdq(ig,l,igcm_h2o_ice) |
|---|
| 482 | subpdq(ig,l,igcm_ccn_mass) = |
|---|
| 483 | & subpdq(ig,l,igcm_ccn_mass) |
|---|
| 484 | & + pdq(ig,l,igcm_ccn_mass) |
|---|
| 485 | subpdq(ig,l,igcm_ccn_number) = |
|---|
| 486 | & subpdq(ig,l,igcm_ccn_number) |
|---|
| 487 | & + pdq(ig,l,igcm_ccn_number) |
|---|
| 488 | ENDDO |
|---|
| 489 | ENDDO |
|---|
| 490 | c- Effective tracers quantities in the cloud fraction |
|---|
| 491 | IF (CLFvaryingCO2) THEN |
|---|
| 492 | pqeff(:,:,:)=pq(:,:,:) ! prevent from buggs (A. Pottier) |
|---|
| 493 | pqeff(:,:,igcm_ccnco2_mass) =pq(:,:,igcm_ccnco2_mass)/ |
|---|
| 494 | & cloudfrac(:,:) |
|---|
| 495 | pqeff(:,:,igcm_ccnco2_number)= |
|---|
| 496 | & pq(:,:,igcm_ccnco2_number)/cloudfrac(:,:) |
|---|
| 497 | pqeff(:,:,igcm_co2_ice)= pq(:,:,igcm_co2_ice)/ |
|---|
| 498 | & cloudfrac(:,:) |
|---|
| 499 | ELSE |
|---|
| 500 | pqeff(:,:,:)=pq(:,:,:) |
|---|
| 501 | END IF |
|---|
| 502 | |
|---|
| 503 | c------------------------------------------------------ |
|---|
| 504 | c 1.SEDIMENTATION : update tracers, compute parameters, |
|---|
| 505 | c call to sedimentation routine, update tendancies |
|---|
| 506 | c------------------------------------------------------ |
|---|
| 507 | DO l=1, nlay |
|---|
| 508 | DO ig=1,ngrid |
|---|
| 509 | tempo_traceur_t(ig,l)=zteff(ig,l)+subpdt(ig,l) |
|---|
| 510 | & *microtimestep |
|---|
| 511 | tempo_traceurs(ig,l,:)=pqeff(ig,l,:) |
|---|
| 512 | & +subpdq(ig,l,:)*microtimestep |
|---|
| 513 | rho_ice_co2T(ig,l)=1000.*(1.72391-2.53e-4* |
|---|
| 514 | & tempo_traceur_t(ig,l)-2.87e-6* |
|---|
| 515 | & tempo_traceur_t(ig,l)*tempo_traceur_t(ig,l)) |
|---|
| 516 | |
|---|
| 517 | rho_ice_co2=rho_ice_co2T(ig,l) |
|---|
| 518 | Niceco2=max(tempo_traceurs(ig,l,igcm_co2_ice),1.e-30) |
|---|
| 519 | Nccnco2=max(tempo_traceurs(ig,l,igcm_ccnco2_number), |
|---|
| 520 | & 1.e-30) |
|---|
| 521 | Qccnco2=max(tempo_traceurs(ig,l,igcm_ccnco2_mass), |
|---|
| 522 | & 1.e-30) |
|---|
| 523 | call updaterice_microco2(Niceco2, |
|---|
| 524 | & Qccnco2,Nccnco2, |
|---|
| 525 | & tauscaling(ig),riceco2(ig,l),rhocloudco2t(ig,l)) |
|---|
| 526 | if (Niceco2 .le. 1.e-25 |
|---|
| 527 | & .or. Nccnco2*tauscaling(ig) .le. 1) THEN |
|---|
| 528 | riceco2(ig,l)=1.e-9 |
|---|
| 529 | endif |
|---|
| 530 | rhocloudco2t(ig,l)=min(max(rhocloudco2t(ig,l) |
|---|
| 531 | & ,rho_ice_co2),rho_dust) |
|---|
| 532 | rsedcloudco2(ig,l)=max(riceco2(ig,l)* |
|---|
| 533 | & (1.+nuiceco2_sed)*(1.+nuiceco2_sed)*(1.+nuiceco2_sed), |
|---|
| 534 | & riceco2(ig,l)) |
|---|
| 535 | ENDDO |
|---|
| 536 | ENDDO |
|---|
| 537 | ! Gravitational sedimentation |
|---|
| 538 | sav_trac(:,:,igcm_co2_ice)=tempo_traceurs(:,:,igcm_co2_ice) |
|---|
| 539 | sav_trac(:,:,igcm_ccnco2_mass)= |
|---|
| 540 | & tempo_traceurs(:,:,igcm_ccnco2_mass) |
|---|
| 541 | sav_trac(:,:,igcm_ccnco2_number)= |
|---|
| 542 | & tempo_traceurs(:,:,igcm_ccnco2_number) |
|---|
| 543 | !We save actualized tracer values to compute sedimentation tendancies |
|---|
| 544 | call newsedim(ngrid,nlay,ngrid*nlay,ngrid*nlay, |
|---|
| 545 | & microtimestep,pplev,masse,epaisseur,tempo_traceur_t, |
|---|
| 546 | & rsedcloudco2,rhocloudco2t, |
|---|
| 547 | & tempo_traceurs(:,:,igcm_co2_ice),wq,beta) ! 3 traceurs |
|---|
| 548 | ! sedim at the surface of co2 ice : keep track of it for physiq_mod |
|---|
| 549 | do ig=1,ngrid |
|---|
| 550 | pdqs_sedco2(ig)=pdqs_sedco2(ig)+ wq(ig,1)/microtimestep |
|---|
| 551 | end do |
|---|
| 552 | call newsedim(ngrid,nlay,ngrid*nlay,ngrid*nlay, |
|---|
| 553 | & microtimestep,pplev,masse,epaisseur,tempo_traceur_t, |
|---|
| 554 | & rsedcloudco2,rhocloudco2t, |
|---|
| 555 | & tempo_traceurs(:,:,igcm_ccnco2_mass),wq,beta) |
|---|
| 556 | call newsedim(ngrid,nlay,ngrid*nlay,ngrid*nlay, |
|---|
| 557 | & microtimestep,pplev,masse,epaisseur,tempo_traceur_t, |
|---|
| 558 | & rsedcloudco2,rhocloudco2t, |
|---|
| 559 | & tempo_traceurs(:,:,igcm_ccnco2_number),wq,beta) |
|---|
| 560 | DO l = 1, nlay !Compute tendencies |
|---|
| 561 | DO ig=1,ngrid |
|---|
| 562 | pdqsed(ig,l,igcm_ccnco2_mass)= |
|---|
| 563 | & (tempo_traceurs(ig,l,igcm_ccnco2_mass)- |
|---|
| 564 | & sav_trac(ig,l,igcm_ccnco2_mass))/microtimestep |
|---|
| 565 | pdqsed(ig,l,igcm_ccnco2_number)= |
|---|
| 566 | & (tempo_traceurs(ig,l,igcm_ccnco2_number)- |
|---|
| 567 | & sav_trac(ig,l,igcm_ccnco2_number))/microtimestep |
|---|
| 568 | pdqsed(ig,l,igcm_co2_ice)= |
|---|
| 569 | & (tempo_traceurs(ig,l,igcm_co2_ice)- |
|---|
| 570 | & sav_trac(ig,l,igcm_co2_ice))/microtimestep |
|---|
| 571 | ENDDO |
|---|
| 572 | ENDDO |
|---|
| 573 | !update subtimestep tendencies with sedimentation input |
|---|
| 574 | DO l=1,nlay |
|---|
| 575 | DO ig=1,ngrid |
|---|
| 576 | subpdq(ig,l,igcm_ccnco2_mass) = |
|---|
| 577 | & subpdq(ig,l,igcm_ccnco2_mass) |
|---|
| 578 | & +pdqsed(ig,l,igcm_ccnco2_mass) |
|---|
| 579 | subpdq(ig,l,igcm_ccnco2_number) = |
|---|
| 580 | & subpdq(ig,l,igcm_ccnco2_number) |
|---|
| 581 | & +pdqsed(ig,l,igcm_ccnco2_number) |
|---|
| 582 | subpdq(ig,l,igcm_co2_ice) = |
|---|
| 583 | & subpdq(ig,l,igcm_co2_ice) |
|---|
| 584 | & +pdqsed(ig,l,igcm_co2_ice) |
|---|
| 585 | ENDDO |
|---|
| 586 | ENDDO |
|---|
| 587 | c------------------------------------------------------ |
|---|
| 588 | c 2. Main call to the cloud schemes: |
|---|
| 589 | c------------------------------------------------------ |
|---|
| 590 | CALL improvedCO2clouds(ngrid,nlay,microtimestep, |
|---|
| 591 | & pplay,pplev,zteff,subpdt, |
|---|
| 592 | & pqeff,subpdq,subpdqcloudco2,subpdtcloudco2, |
|---|
| 593 | & nq,tauscaling,memdMMccn,memdMMh2o,memdNNccn) |
|---|
| 594 | c----------------------------------------------------- |
|---|
| 595 | c 3. Updating tendencies after cloud scheme: |
|---|
| 596 | c----------------------------------------------------- |
|---|
| 597 | DO l=1,nlay |
|---|
| 598 | DO ig=1,ngrid |
|---|
| 599 | subpdt(ig,l) = |
|---|
| 600 | & subpdt(ig,l) + subpdtcloudco2(ig,l) |
|---|
| 601 | |
|---|
| 602 | subpdq(ig,l,igcm_dust_mass) = |
|---|
| 603 | & subpdq(ig,l,igcm_dust_mass) |
|---|
| 604 | & + subpdqcloudco2(ig,l,igcm_dust_mass) |
|---|
| 605 | subpdq(ig,l,igcm_dust_number) = |
|---|
| 606 | & subpdq(ig,l,igcm_dust_number) |
|---|
| 607 | & + subpdqcloudco2(ig,l,igcm_dust_number) |
|---|
| 608 | |
|---|
| 609 | subpdq(ig,l,igcm_ccnco2_mass) = |
|---|
| 610 | & subpdq(ig,l,igcm_ccnco2_mass) |
|---|
| 611 | & + subpdqcloudco2(ig,l,igcm_ccnco2_mass) |
|---|
| 612 | subpdq(ig,l,igcm_ccnco2_number) = |
|---|
| 613 | & subpdq(ig,l,igcm_ccnco2_number) |
|---|
| 614 | & + subpdqcloudco2(ig,l,igcm_ccnco2_number) |
|---|
| 615 | |
|---|
| 616 | subpdq(ig,l,igcm_co2_ice) = |
|---|
| 617 | & subpdq(ig,l,igcm_co2_ice) |
|---|
| 618 | & + subpdqcloudco2(ig,l,igcm_co2_ice) |
|---|
| 619 | subpdq(ig,l,igcm_co2) = |
|---|
| 620 | & subpdq(ig,l,igcm_co2) |
|---|
| 621 | & + subpdqcloudco2(ig,l,igcm_co2) |
|---|
| 622 | |
|---|
| 623 | subpdq(ig,l,igcm_h2o_ice) = |
|---|
| 624 | & subpdq(ig,l,igcm_h2o_ice) |
|---|
| 625 | & + subpdqcloudco2(ig,l,igcm_h2o_ice) |
|---|
| 626 | subpdq(ig,l,igcm_ccn_mass) = |
|---|
| 627 | & subpdq(ig,l,igcm_ccn_mass) |
|---|
| 628 | & + subpdqcloudco2(ig,l,igcm_ccn_mass) |
|---|
| 629 | subpdq(ig,l,igcm_ccn_number) = |
|---|
| 630 | & subpdq(ig,l,igcm_ccn_number) |
|---|
| 631 | & + subpdqcloudco2(ig,l,igcm_ccn_number) |
|---|
| 632 | ENDDO |
|---|
| 633 | ENDDO |
|---|
| 634 | ENDDO ! of DO microstep=1,imicro |
|---|
| 635 | |
|---|
| 636 | c------------------------------------------------ |
|---|
| 637 | c Compute final tendencies after time loop: |
|---|
| 638 | c------------------------------------------------ |
|---|
| 639 | c CO2 flux at surface (kg.m-2.s-1) |
|---|
| 640 | do ig=1,ngrid |
|---|
| 641 | pdqs_sedco2(ig)=pdqs_sedco2(ig)/real(imicroco2) |
|---|
| 642 | enddo |
|---|
| 643 | c------ Temperature tendency pdtcloud |
|---|
| 644 | DO l=1,nlay |
|---|
| 645 | DO ig=1,ngrid |
|---|
| 646 | pdtcloudco2(ig,l) = |
|---|
| 647 | & subpdt(ig,l)/real(imicroco2)-pdt(ig,l) |
|---|
| 648 | ENDDO |
|---|
| 649 | ENDDO |
|---|
| 650 | c------ Tracers tendencies pdqcloud |
|---|
| 651 | DO l=1,nlay |
|---|
| 652 | DO ig=1,ngrid |
|---|
| 653 | pdqcloudco2(ig,l,igcm_co2_ice) = |
|---|
| 654 | & subpdq(ig,l,igcm_co2_ice)/real(imicroco2) |
|---|
| 655 | & - pdq(ig,l,igcm_co2_ice) |
|---|
| 656 | pdqcloudco2(ig,l,igcm_co2) = |
|---|
| 657 | & subpdq(ig,l,igcm_co2)/real(imicroco2) |
|---|
| 658 | & - pdq(ig,l,igcm_co2) |
|---|
| 659 | pdqcloudco2(ig,l,igcm_h2o_ice) = |
|---|
| 660 | & subpdq(ig,l,igcm_h2o_ice)/real(imicroco2) |
|---|
| 661 | & - pdq(ig,l,igcm_h2o_ice) |
|---|
| 662 | ENDDO |
|---|
| 663 | ENDDO |
|---|
| 664 | DO l=1,nlay |
|---|
| 665 | DO ig=1,ngrid |
|---|
| 666 | pdqcloudco2(ig,l,igcm_ccnco2_mass) = |
|---|
| 667 | & subpdq(ig,l,igcm_ccnco2_mass)/real(imicroco2) |
|---|
| 668 | & - pdq(ig,l,igcm_ccnco2_mass) |
|---|
| 669 | pdqcloudco2(ig,l,igcm_ccnco2_number) = |
|---|
| 670 | & subpdq(ig,l,igcm_ccnco2_number)/real(imicroco2) |
|---|
| 671 | & - pdq(ig,l,igcm_ccnco2_number) |
|---|
| 672 | pdqcloudco2(ig,l,igcm_ccn_mass) = |
|---|
| 673 | & subpdq(ig,l,igcm_ccn_mass)/real(imicroco2) |
|---|
| 674 | & - pdq(ig,l,igcm_ccn_mass) |
|---|
| 675 | pdqcloudco2(ig,l,igcm_ccn_number) = |
|---|
| 676 | & subpdq(ig,l,igcm_ccn_number)/real(imicroco2) |
|---|
| 677 | & - pdq(ig,l,igcm_ccn_number) |
|---|
| 678 | ENDDO |
|---|
| 679 | ENDDO |
|---|
| 680 | DO l=1,nlay |
|---|
| 681 | DO ig=1,ngrid |
|---|
| 682 | pdqcloudco2(ig,l,igcm_dust_mass) = |
|---|
| 683 | & subpdq(ig,l,igcm_dust_mass)/real(imicroco2) |
|---|
| 684 | & - pdq(ig,l,igcm_dust_mass) |
|---|
| 685 | pdqcloudco2(ig,l,igcm_dust_number) = |
|---|
| 686 | & subpdq(ig,l,igcm_dust_number)/real(imicroco2) |
|---|
| 687 | & - pdq(ig,l,igcm_dust_number) |
|---|
| 688 | ENDDO |
|---|
| 689 | ENDDO |
|---|
| 690 | c-------Due to stepped entry, other processes tendencies can add up to negative values |
|---|
| 691 | c-------Therefore, enforce positive values and conserve mass |
|---|
| 692 | DO l=1,nlay |
|---|
| 693 | DO ig=1,ngrid |
|---|
| 694 | IF ((pqeff(ig,l,igcm_ccnco2_number) + |
|---|
| 695 | & ptimestep* (pdq(ig,l,igcm_ccnco2_number) + |
|---|
| 696 | & pdqcloudco2(ig,l,igcm_ccnco2_number)) |
|---|
| 697 | & .lt. 1.) |
|---|
| 698 | & .or. (pqeff(ig,l,igcm_ccnco2_mass) + |
|---|
| 699 | & ptimestep* (pdq(ig,l,igcm_ccnco2_mass) + |
|---|
| 700 | & pdqcloudco2(ig,l,igcm_ccnco2_mass)) |
|---|
| 701 | & .lt. 1.e-20)) THEN |
|---|
| 702 | pdqcloudco2(ig,l,igcm_ccnco2_number) = |
|---|
| 703 | & - pqeff(ig,l,igcm_ccnco2_number)/ptimestep |
|---|
| 704 | & - pdq(ig,l,igcm_ccnco2_number)+1. |
|---|
| 705 | pdqcloudco2(ig,l,igcm_dust_number) = |
|---|
| 706 | & -pdqcloudco2(ig,l,igcm_ccnco2_number) |
|---|
| 707 | pdqcloudco2(ig,l,igcm_ccnco2_mass) = |
|---|
| 708 | & - pqeff(ig,l,igcm_ccnco2_mass)/ptimestep |
|---|
| 709 | & - pdq(ig,l,igcm_ccnco2_mass)+1.e-20 |
|---|
| 710 | pdqcloudco2(ig,l,igcm_dust_mass) = |
|---|
| 711 | & -pdqcloudco2(ig,l,igcm_ccnco2_mass) |
|---|
| 712 | ENDIF |
|---|
| 713 | ENDDO |
|---|
| 714 | ENDDO |
|---|
| 715 | DO l=1,nlay |
|---|
| 716 | DO ig=1,ngrid |
|---|
| 717 | IF ( (pqeff(ig,l,igcm_dust_number) + |
|---|
| 718 | & ptimestep* (pdq(ig,l,igcm_dust_number) + |
|---|
| 719 | & pdqcloudco2(ig,l,igcm_dust_number)) .le. 1.) |
|---|
| 720 | & .or. (pqeff(ig,l,igcm_dust_mass)+ |
|---|
| 721 | & ptimestep* (pdq(ig,l,igcm_dust_mass) + |
|---|
| 722 | & pdqcloudco2(ig,l,igcm_dust_mass)) |
|---|
| 723 | & .le. 1.e-20)) then |
|---|
| 724 | pdqcloudco2(ig,l,igcm_dust_number) = |
|---|
| 725 | & - pqeff(ig,l,igcm_dust_number)/ptimestep |
|---|
| 726 | & - pdq(ig,l,igcm_dust_number)+1. |
|---|
| 727 | pdqcloudco2(ig,l,igcm_ccnco2_number) = |
|---|
| 728 | & -pdqcloudco2(ig,l,igcm_dust_number) |
|---|
| 729 | pdqcloudco2(ig,l,igcm_dust_mass) = |
|---|
| 730 | & - pqeff(ig,l,igcm_dust_mass)/ptimestep |
|---|
| 731 | & - pdq(ig,l,igcm_dust_mass) +1.e-20 |
|---|
| 732 | pdqcloudco2(ig,l,igcm_ccnco2_mass) = |
|---|
| 733 | & -pdqcloudco2(ig,l,igcm_dust_mass) |
|---|
| 734 | ENDIF |
|---|
| 735 | ENDDO |
|---|
| 736 | ENDDO |
|---|
| 737 | !pq+ptime*(pdq+pdqc)=1 ! pdqc=1-pq/ptime-pdq |
|---|
| 738 | DO l=1,nlay |
|---|
| 739 | DO ig=1,ngrid |
|---|
| 740 | IF (pqeff(ig,l,igcm_co2_ice) + ptimestep* |
|---|
| 741 | & (pdq(ig,l,igcm_co2_ice) + pdqcloudco2(ig,l,igcm_co2_ice)) |
|---|
| 742 | & .lt. 1.e-15) THEN |
|---|
| 743 | pdqcloudco2(ig,l,igcm_co2_ice) = |
|---|
| 744 | & - pqeff(ig,l,igcm_co2_ice)/ptimestep-pdq(ig,l,igcm_co2_ice) |
|---|
| 745 | pdqcloudco2(ig,l,igcm_co2) = -pdqcloudco2(ig,l,igcm_co2_ice) |
|---|
| 746 | ENDIF |
|---|
| 747 | IF (pqeff(ig,l,igcm_co2) + ptimestep* |
|---|
| 748 | & (pdq(ig,l,igcm_co2) + pdqcloudco2(ig,l,igcm_co2)) |
|---|
| 749 | & .lt. 0.1) THEN |
|---|
| 750 | pdqcloudco2(ig,l,igcm_co2) = |
|---|
| 751 | & - pqeff(ig,l,igcm_co2)/ptimestep - pdq(ig,l,igcm_co2) |
|---|
| 752 | pdqcloudco2(ig,l,igcm_co2_ice)= -pdqcloudco2(ig,l,igcm_co2) |
|---|
| 753 | ENDIF |
|---|
| 754 | ENDDO |
|---|
| 755 | ENDDO |
|---|
| 756 | |
|---|
| 757 | c Update clouds parameters values in the cloud fraction (for output) |
|---|
| 758 | DO l=1, nlay |
|---|
| 759 | DO ig=1,ngrid |
|---|
| 760 | |
|---|
| 761 | Niceco2=pqeff(ig,l,igcm_co2_ice) + |
|---|
| 762 | & (pdq(ig,l,igcm_co2_ice) + |
|---|
| 763 | & pdqcloudco2(ig,l,igcm_co2_ice))*ptimestep |
|---|
| 764 | Nco2=pqeff(ig,l,igcm_co2) + |
|---|
| 765 | & (pdq(ig,l,igcm_co2) + |
|---|
| 766 | & pdqcloudco2(ig,l,igcm_co2))*ptimestep |
|---|
| 767 | Nccnco2=max((pqeff(ig,l,igcm_ccnco2_number) + |
|---|
| 768 | & (pdq(ig,l,igcm_ccnco2_number) + |
|---|
| 769 | & pdqcloudco2(ig,l,igcm_ccnco2_number))*ptimestep) |
|---|
| 770 | & ,1.e-30) |
|---|
| 771 | Qccnco2=max((pqeff(ig,l,igcm_ccnco2_mass) + |
|---|
| 772 | & (pdq(ig,l,igcm_ccnco2_mass) + |
|---|
| 773 | & pdqcloudco2(ig,l,igcm_ccnco2_mass))*ptimestep) |
|---|
| 774 | & ,1.e-30) |
|---|
| 775 | |
|---|
| 776 | myT=zteff(ig,l)+(pdt(ig,l)+pdtcloudco2(ig,l))*ptimestep |
|---|
| 777 | rho_ice_co2T(ig,l)=1000.*(1.72391-2.53e-4* |
|---|
| 778 | & myT-2.87e-6* myT* myT) |
|---|
| 779 | rho_ice_co2=rho_ice_co2T(ig,l) |
|---|
| 780 | c rho_ice_co2 is shared by tracer_mod and used in updaterice |
|---|
| 781 | c Compute particle size |
|---|
| 782 | call updaterice_microco2(Niceco2, |
|---|
| 783 | & Qccnco2,Nccnco2, |
|---|
| 784 | & tauscaling(ig),riceco2(ig,l),rhocloudco2(ig,l)) |
|---|
| 785 | |
|---|
| 786 | if ( (Niceco2 .le. 1.e-25 .or. |
|---|
| 787 | & Nccnco2*tauscaling(ig) .le. 1.) )THEN |
|---|
| 788 | riceco2(ig,l)=0. |
|---|
| 789 | endif |
|---|
| 790 | c Compute opacities |
|---|
| 791 | No=Nccnco2*tauscaling(ig) |
|---|
| 792 | Rn=-dlog(riceco2(ig,l)) |
|---|
| 793 | n_derf = derf( (rb_cldco2(1)+Rn) *dev2) |
|---|
| 794 | Qext1bins2(ig,l)=0. |
|---|
| 795 | do i = 1, nbinco2_cld |
|---|
| 796 | n_aer(i) = -0.5 * No * n_derf !! this ith previously computed |
|---|
| 797 | n_derf = derf((rb_cldco2(i+1)+Rn) *dev2) |
|---|
| 798 | n_aer(i) = n_aer(i) + 0.5 * No * n_derf |
|---|
| 799 | Qext1bins2(ig,l)=Qext1bins2(ig,l)+Qext1bins(i)*n_aer(i) |
|---|
| 800 | enddo |
|---|
| 801 | |
|---|
| 802 | !update rice water |
|---|
| 803 | call updaterice_micro( |
|---|
| 804 | & pqeff(ig,l,igcm_h2o_ice) + ! ice mass |
|---|
| 805 | & (pdq(ig,l,igcm_h2o_ice) + ! ice mass |
|---|
| 806 | & pdqcloudco2(ig,l,igcm_h2o_ice))*ptimestep, ! ice mass |
|---|
| 807 | & pqeff(ig,l,igcm_ccn_mass) + ! ccn mass |
|---|
| 808 | & (pdq(ig,l,igcm_ccn_mass) + ! ccn mass |
|---|
| 809 | & pdqcloudco2(ig,l,igcm_ccn_mass))*ptimestep, ! ccn mass |
|---|
| 810 | & pqeff(ig,l,igcm_ccn_number) + ! ccn number |
|---|
| 811 | & (pdq(ig,l,igcm_ccn_number) + ! ccn number |
|---|
| 812 | & pdqcloudco2(ig,l,igcm_ccn_number))*ptimestep, ! ccn number |
|---|
| 813 | & tauscaling(ig),rice(ig,l),rhocloud(ig,l)) |
|---|
| 814 | |
|---|
| 815 | call updaterdust( |
|---|
| 816 | & pqeff(ig,l,igcm_dust_mass) + ! dust mass |
|---|
| 817 | & (pdq(ig,l,igcm_dust_mass) + ! dust mass |
|---|
| 818 | & pdqcloudco2(ig,l,igcm_dust_mass))*ptimestep, ! dust mass |
|---|
| 819 | & pqeff(ig,l,igcm_dust_number) + ! dust number |
|---|
| 820 | & (pdq(ig,l,igcm_dust_number) + ! dust number |
|---|
| 821 | & pdqcloudco2(ig,l,igcm_dust_number))*ptimestep, ! dust number |
|---|
| 822 | & rdust(ig,l)) |
|---|
| 823 | |
|---|
| 824 | ENDDO |
|---|
| 825 | ENDDO |
|---|
| 826 | |
|---|
| 827 | c A correction if a lot of subliming CO2 fills the 1st layer FF04/2005 |
|---|
| 828 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
|---|
| 829 | c Then that should not affect the ice particle radius |
|---|
| 830 | |
|---|
| 831 | do ig=1,ngrid |
|---|
| 832 | if(pdpsrf(ig)*ptimestep.gt.0.9*(pplev(ig,1)-pplev(ig,2)))then |
|---|
| 833 | if(pdpsrf(ig)*ptimestep.gt.0.9*(pplev(ig,1)-pplev(ig,3))) |
|---|
| 834 | & riceco2(ig,2)=riceco2(ig,3) |
|---|
| 835 | riceco2(ig,1)=riceco2(ig,2) |
|---|
| 836 | end if |
|---|
| 837 | end do |
|---|
| 838 | |
|---|
| 839 | DO l=1,nlay |
|---|
| 840 | DO ig=1,ngrid |
|---|
| 841 | rsedcloud(ig,l)=max(rice(ig,l)* |
|---|
| 842 | & (1.+nuice_sed)*(1.+nuice_sed)*(1.+nuice_sed), |
|---|
| 843 | & rdust(ig,l)) |
|---|
| 844 | ! rsedcloud(ig,l)=min(rsedcloud(ig,l),1.e-4) |
|---|
| 845 | ENDDO |
|---|
| 846 | ENDDO |
|---|
| 847 | |
|---|
| 848 | DO l=1,nlay |
|---|
| 849 | DO ig=1,ngrid |
|---|
| 850 | rsedcloudco2(ig,l)=max(riceco2(ig,l)* |
|---|
| 851 | & (1.+nuiceco2_sed)*(1.+nuiceco2_sed)*(1.+nuiceco2_sed), |
|---|
| 852 | & rdust(ig,l)) |
|---|
| 853 | c rsedcloudco2(ig,l)=min(rsedcloudco2(ig,l),1.e-5) |
|---|
| 854 | ENDDO |
|---|
| 855 | ENDDO |
|---|
| 856 | |
|---|
| 857 | call co2sat(ngrid*nlay,zteff+(pdt+pdtcloudco2)*ptimestep |
|---|
| 858 | & ,pplay,zqsatco2) |
|---|
| 859 | do l=1,nlay |
|---|
| 860 | do ig=1,ngrid |
|---|
| 861 | satuco2(ig,l) = (pqeff(ig,l,igcm_co2) + |
|---|
| 862 | & (pdq(ig,l,igcm_co2) + |
|---|
| 863 | & pdqcloudco2(ig,l,igcm_co2))*ptimestep)* |
|---|
| 864 | & (mmean(ig,l)/44.01)*pplay(ig,l)/zqsatco2(ig,l) |
|---|
| 865 | enddo |
|---|
| 866 | enddo |
|---|
| 867 | !Tout ce qui est modifié par la microphysique de CO2 doit être rapporté a cloudfrac |
|---|
| 868 | IF (CLFvaryingCO2) THEN |
|---|
| 869 | DO l=1,nlay |
|---|
| 870 | DO ig=1,ngrid |
|---|
| 871 | pdqcloudco2(ig,l,igcm_ccn_mass)= |
|---|
| 872 | & pdqcloudco2(ig,l,igcm_ccn_mass)*cloudfrac(ig,l) |
|---|
| 873 | pdqcloudco2(ig,l,igcm_ccnco2_mass)= |
|---|
| 874 | & pdqcloudco2(ig,l,igcm_ccnco2_mass)*cloudfrac(ig,l) |
|---|
| 875 | pdqcloudco2(ig,l,igcm_ccn_number)= |
|---|
| 876 | & pdqcloudco2(ig,l,igcm_ccn_number)*cloudfrac(ig,l) |
|---|
| 877 | pdqcloudco2(ig,l,igcm_ccnco2_number)= |
|---|
| 878 | & pdqcloudco2(ig,l,igcm_ccnco2_number)*cloudfrac(ig,l) |
|---|
| 879 | pdqcloudco2(ig,l,igcm_dust_mass)= |
|---|
| 880 | & pdqcloudco2(ig,l,igcm_dust_mass)*cloudfrac(ig,l) |
|---|
| 881 | pdqcloudco2(ig,l,igcm_dust_number)= |
|---|
| 882 | & pdqcloudco2(ig,l,igcm_dust_number)*cloudfrac(ig,l) |
|---|
| 883 | pdqcloudco2(ig,l,igcm_h2o_ice)= |
|---|
| 884 | & pdqcloudco2(ig,l,igcm_h2o_ice)*cloudfrac(ig,l) |
|---|
| 885 | pdqcloudco2(ig,l,igcm_co2_ice)= |
|---|
| 886 | & pdqcloudco2(ig,l,igcm_co2_ice)*cloudfrac(ig,l) |
|---|
| 887 | pdqcloudco2(ig,l,igcm_co2)= |
|---|
| 888 | & pdqcloudco2(ig,l,igcm_co2)*cloudfrac(ig,l) |
|---|
| 889 | pdtcloudco2(ig,l)=pdtcloudco2(ig,l)*cloudfrac(ig,l) |
|---|
| 890 | Qext1bins2(ig,l)=Qext1bins2(ig,l)*cloudfrac(ig,l) |
|---|
| 891 | ENDDO |
|---|
| 892 | ENDDO |
|---|
| 893 | ENDIF |
|---|
| 894 | !l'opacité de la case ig est la somme sur l de Qext1bins2: Est-ce-vrai? |
|---|
| 895 | tau1mic(:)=0. |
|---|
| 896 | do l=1,nlay |
|---|
| 897 | do ig=1,ngrid |
|---|
| 898 | tau1mic(ig)=tau1mic(ig)+Qext1bins2(ig,l) |
|---|
| 899 | enddo |
|---|
| 900 | enddo |
|---|
| 901 | !Outputs: |
|---|
| 902 | call WRITEDIAGFI(ngrid,"SatIndex","SatIndex"," ",3, |
|---|
| 903 | & SatIndex) |
|---|
| 904 | call WRITEDIAGFI(ngrid,"satuco2","vap in satu","kg/kg",3, |
|---|
| 905 | & satuco2) |
|---|
| 906 | call WRITEdiagfi(ngrid,"riceco2","ice radius","m" |
|---|
| 907 | & ,3,riceco2) |
|---|
| 908 | call WRITEdiagfi(ngrid,"cloudfrac","co2 cloud fraction" |
|---|
| 909 | & ," ",3,cloudfrac) |
|---|
| 910 | call WRITEdiagfi(ngrid,"rsedcloudco2","rsed co2" |
|---|
| 911 | & ,"m",3,rsedcloudco2) |
|---|
| 912 | call WRITEdiagfi(ngrid,"Tau3D1mic"," co2 ice opacities" |
|---|
| 913 | & ," ",3,Qext1bins2) |
|---|
| 914 | call WRITEdiagfi(ngrid,"tau1mic","co2 ice opacity 1 micron" |
|---|
| 915 | & ," ",2,tau1mic) |
|---|
| 916 | |
|---|
| 917 | END |
|---|