[358] | 1 | subroutine improvedclouds(ngrid,nlay,ptimestep, |
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[520] | 2 | & pplev,pplay,zlev,pt,pdt, |
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| 3 | & pq,pdq,pdqcloud,pdtcloud, |
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[358] | 4 | & nq,tauscaling,rdust,rice,nuice, |
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| 5 | & rsedcloud,rhocloud) |
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[520] | 6 | ! to use 'getin' |
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| 7 | USE ioipsl_getincom |
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[358] | 8 | implicit none |
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| 9 | c------------------------------------------------------------------ |
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| 10 | c This routine is used to form clouds when a parcel of the GCM is |
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| 11 | c saturated. It includes the ability to have supersaturation, a |
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| 12 | c computation of the nucleation rates, growthrates and the |
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| 13 | c scavenging of dust particles by clouds. |
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| 14 | c It is worth noting that the amount of dust is computed using the |
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| 15 | c dust optical depth computed in aeropacity.F. That's why |
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| 16 | c the variable called "tauscaling" is used to convert |
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| 17 | c pq(dust_mass) and pq(dust_number), which are relative |
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| 18 | c quantities, to absolute and realistic quantities stored in zq. |
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| 19 | c This has to be done to convert the inputs into absolute |
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| 20 | c values, but also to convert the outputs back into relative |
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| 21 | c values which are then used by the sedimentation and advection |
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| 22 | c schemes. |
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| 23 | |
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| 24 | c Authors: J.-B. Madeleine, based on the work by Franck Montmessin |
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| 25 | c (October 2011) |
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[520] | 26 | c T. Navarro, debug & correction (October-December 2011) |
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[530] | 27 | c A. Spiga, optimization (February 2012) |
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[358] | 28 | c------------------------------------------------------------------ |
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| 29 | #include "dimensions.h" |
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| 30 | #include "dimphys.h" |
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| 31 | #include "comcstfi.h" |
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| 32 | #include "callkeys.h" |
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| 33 | #include "tracer.h" |
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| 34 | #include "comgeomfi.h" |
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| 35 | #include "dimradmars.h" |
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| 36 | #include "microphys.h" |
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| 37 | c------------------------------------------------------------------ |
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| 38 | c Inputs: |
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| 39 | |
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| 40 | INTEGER ngrid,nlay |
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| 41 | integer nq ! nombre de traceurs |
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| 42 | REAL ptimestep ! pas de temps physique (s) |
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[520] | 43 | REAL pplev(ngrid,nlay+1) ! pression aux inter-couches (Pa) |
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| 44 | REAL pplay(ngrid,nlay) ! pression au milieu des couches (Pa) |
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| 45 | REAL zlev(ngrid,nlay+1) ! altitude at layer boundaries |
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| 46 | |
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[358] | 47 | REAL pt(ngrid,nlay) ! temperature at the middle of the |
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| 48 | ! layers (K) |
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| 49 | REAL pdt(ngrid,nlay) ! tendance temperature des autres |
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| 50 | ! param. |
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| 51 | REAL pq(ngrid,nlay,nq) ! traceur (kg/kg) |
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| 52 | REAL pdq(ngrid,nlay,nq) ! tendance avant condensation |
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| 53 | ! (kg/kg.s-1) |
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| 54 | REAL tauscaling(ngridmx) ! Convertion factor for qdust and Ndust |
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| 55 | REAL rdust(ngridmx,nlayermx) ! Dust geometric mean radius (m) |
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| 56 | |
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| 57 | c Outputs: |
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| 58 | REAL rice(ngrid,nlay) ! Ice mass mean radius (m) |
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| 59 | ! (r_c in montmessin_2004) |
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| 60 | REAL nuice(ngrid,nlay) ! Estimated effective variance |
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| 61 | ! of the size distribution |
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| 62 | REAL rsedcloud(ngridmx,nlayermx) ! Cloud sedimentation radius |
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| 63 | REAL rhocloud(ngridmx,nlayermx) ! Cloud density (kg.m-3) |
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| 64 | REAL pdqcloud(ngrid,nlay,nq) ! tendance de la condensation |
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| 65 | ! H2O(kg/kg.s-1) |
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| 66 | REAL pdtcloud(ngrid,nlay) ! tendance temperature due |
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| 67 | ! a la chaleur latente |
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| 68 | |
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| 69 | c------------------------------------------------------------------ |
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| 70 | c Local variables: |
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| 71 | |
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| 72 | LOGICAL firstcall |
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| 73 | DATA firstcall/.true./ |
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| 74 | SAVE firstcall |
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| 75 | |
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| 76 | REAL*8 derf ! Error function |
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| 77 | !external derf |
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| 78 | |
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| 79 | REAL CBRT |
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| 80 | EXTERNAL CBRT |
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| 81 | |
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| 82 | INTEGER ig,l,i |
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[520] | 83 | |
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[358] | 84 | |
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| 85 | REAL zq(ngridmx,nlayermx,nqmx) ! local value of tracers |
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| 86 | REAL zq0(ngridmx,nlayermx,nqmx) ! local initial value of tracers |
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| 87 | REAL zt(ngridmx,nlayermx) ! local value of temperature |
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| 88 | REAL zqsat(ngridmx,nlayermx) ! saturation |
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| 89 | REAL lw !Latent heat of sublimation (J.kg-1) |
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| 90 | REAL Cste |
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| 91 | REAL dMice ! mass of condensated ice |
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| 92 | REAL sumcheck |
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| 93 | REAL*8 ph2o ! Water vapor partial pressure (Pa) |
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| 94 | REAL*8 satu ! Water vapor saturation ratio over ice |
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| 95 | REAL*8 Mo,No |
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| 96 | REAL*8 dN,dM,newvap |
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[530] | 97 | REAL*8 Rn, Rm, dev2, yeah, yeahn, yeahm |
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[358] | 98 | REAL*8 n_aer(nbin_cld) ! number conc. of particle/each size bin |
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| 99 | REAL*8 m_aer(nbin_cld) ! mass mixing ratio of particle/each size bin |
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| 100 | REAL*8 rate(nbin_cld) ! nucleation rate |
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| 101 | REAL*8 up,dwn,Ctot,gr,seq |
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| 102 | REAL*8 sig ! Water-ice/air surface tension (N.m) |
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| 103 | EXTERNAL sig |
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| 104 | |
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| 105 | c Parameters of the size discretization |
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| 106 | c used by the microphysical scheme |
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| 107 | DOUBLE PRECISION, PARAMETER :: rmin_cld = 0.1e-6 ! Minimum radius (m) |
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| 108 | DOUBLE PRECISION, PARAMETER :: rmax_cld = 10.e-6 ! Maximum radius (m) |
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| 109 | DOUBLE PRECISION, PARAMETER :: rbmin_cld = 0.0001e-6 |
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| 110 | ! Minimum boundary radius (m) |
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| 111 | DOUBLE PRECISION, PARAMETER :: rbmax_cld = 1.e-2 ! Maximum boundary radius (m) |
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| 112 | DOUBLE PRECISION vrat_cld ! Volume ratio |
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| 113 | DOUBLE PRECISION rb_cld(nbin_cld+1)! boundary values of each rad_cld bin (m) |
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| 114 | SAVE rb_cld |
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[520] | 115 | DOUBLE PRECISION dr_cld(nbin_cld) ! width of each rad_cld bin (m) |
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| 116 | DOUBLE PRECISION vol_cld(nbin_cld) ! particle volume for each bin (m3) |
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[358] | 117 | |
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| 118 | REAL sigma_ice ! Variance of the ice and CCN distributions |
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| 119 | SAVE sigma_ice |
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[520] | 120 | |
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[420] | 121 | c---------------------------------- |
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| 122 | c some outputs for 1D -- TEMPORARY |
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[358] | 123 | REAL satu_out(ngridmx,nlayermx) ! satu ratio for output |
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| 124 | REAL dN_out(ngridmx,nlayermx) ! mass variation for output |
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| 125 | REAL dM_out(ngridmx,nlayermx) ! number variation for output |
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[411] | 126 | REAL dM_col(ngridmx) ! total mass condensed in column |
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| 127 | REAL dN_col(ngridmx) ! total mass condensed in column |
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[358] | 128 | REAL Mcon_out(ngridmx,nlayermx) ! mass to be condensed (not dMice !!) |
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| 129 | REAL gr_out(ngridmx,nlayermx) ! for 1d output |
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| 130 | REAL newvap_out(ngridmx,nlayermx) ! for 1d output |
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[411] | 131 | REAL Mdust_col(ngridmx) ! total column dust mass |
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| 132 | REAL Ndust_col(ngridmx) ! total column dust mass |
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| 133 | REAL Mccn_col(ngridmx) ! total column ccn mass |
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| 134 | REAL Nccn_col(ngridmx) ! total column ccn mass |
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[520] | 135 | REAL dMice_col(ngridmx) ! total column ice mass change |
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| 136 | REAL drice_col(ngridmx) ! total column ice radius change |
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| 137 | REAL icetot(ngridmx) ! total column ice mass |
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| 138 | REAL rice_out(ngridmx,nlayermx) ! ice radius change |
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[455] | 139 | REAL rate_out(ngridmx,nlayermx) ! nucleation rate |
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[420] | 140 | INTEGER count |
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| 141 | |
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| 142 | LOGICAL output_sca ! scavenging outputs flag for tests |
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[520] | 143 | |
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[420] | 144 | output_sca = .false. |
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| 145 | c---------------------------------- |
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| 146 | c---------------------------------- |
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[358] | 147 | |
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| 148 | c------------------------------------------------------------------ |
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| 149 | |
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| 150 | IF (firstcall) THEN |
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| 151 | |
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| 152 | c Definition of the size grid |
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| 153 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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| 154 | c rad_cld is the primary radius grid used for microphysics computation. |
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| 155 | c The grid spacing is computed assuming a constant volume ratio |
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| 156 | c between two consecutive bins; i.e. vrat_cld. |
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| 157 | c vrat_cld is determined from the boundary values of the size grid: |
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| 158 | c rmin_cld and rmax_cld. |
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| 159 | c The rb_cld array contains the boundary values of each rad_cld bin. |
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| 160 | c dr_cld is the width of each rad_cld bin. |
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| 161 | |
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| 162 | c Volume ratio between two adjacent bins |
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| 163 | vrat_cld = dlog(rmax_cld/rmin_cld) / float(nbin_cld-1) *3. |
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| 164 | vrat_cld = dexp(vrat_cld) |
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| 165 | write(*,*) "vrat_cld", vrat_cld |
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| 166 | |
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| 167 | rb_cld(1) = rbmin_cld |
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| 168 | rad_cld(1) = rmin_cld |
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[530] | 169 | vol_cld(1) = 4./3. * dble(pi) * rmin_cld*rmin_cld*rmin_cld |
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[358] | 170 | |
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| 171 | do i=1,nbin_cld-1 |
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[531] | 172 | rad_cld(i+1) = rad_cld(i) * vrat_cld**(1./3.) |
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[358] | 173 | vol_cld(i+1) = vol_cld(i) * vrat_cld |
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| 174 | enddo |
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| 175 | |
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| 176 | do i=1,nbin_cld |
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[531] | 177 | rb_cld(i+1)= ( (2.*vrat_cld) / (vrat_cld+1.) )**(1./3.) * |
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[358] | 178 | & rad_cld(i) |
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| 179 | dr_cld(i) = rb_cld(i+1) - rb_cld(i) |
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| 180 | enddo |
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| 181 | rb_cld(nbin_cld+1) = rbmax_cld |
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| 182 | dr_cld(nbin_cld) = rb_cld(nbin_cld+1) - rb_cld(nbin_cld) |
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| 183 | |
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| 184 | print*, ' ' |
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| 185 | print*,'Microphysics: size bin information:' |
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| 186 | print*,'i,rb_cld(i), rad_cld(i),dr_cld(i)' |
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| 187 | print*,'-----------------------------------' |
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| 188 | do i=1,nbin_cld |
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| 189 | write(*,'(i2,3x,3(e12.6,4x))') i,rb_cld(i), rad_cld(i), |
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| 190 | & dr_cld(i) |
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| 191 | enddo |
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| 192 | write(*,'(i2,3x,e12.6)') nbin_cld+1,rb_cld(nbin_cld+1) |
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| 193 | print*,'-----------------------------------' |
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| 194 | |
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[541] | 195 | do i=1,nbin_cld+1 |
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| 196 | rb_cld(i) = dlog(rb_cld(i)) !! we save that so that it is not computed |
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| 197 | !! at each timestep and gridpoint |
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| 198 | enddo |
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| 199 | |
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[358] | 200 | c Contact parameter of water ice on dust ( m=cos(theta) ) |
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| 201 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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| 202 | ! mteta = 0.95 |
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| 203 | write(*,*) 'water_param contact parameter:', mteta |
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| 204 | |
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| 205 | c Volume of a water molecule (m3) |
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| 206 | vo1 = mh2o / dble(rho_ice) |
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| 207 | c Variance of the ice and CCN distributions |
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| 208 | sigma_ice = sqrt(log(1.+nuice_sed)) |
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| 209 | |
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| 210 | write(*,*) 'Variance of ice & CCN distribs :', sigma_ice |
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[455] | 211 | write(*,*) 'nuice for sedimentation:', nuice_sed |
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[358] | 212 | write(*,*) 'Volume of a water molecule:', vo1 |
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| 213 | |
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| 214 | firstcall=.false. |
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| 215 | END IF |
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| 216 | |
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| 217 | c----------------------------------------------------------------------- |
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| 218 | c 1. Initialization |
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| 219 | c----------------------------------------------------------------------- |
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[411] | 220 | c Initialize the tendencies |
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| 221 | pdqcloud(1:ngrid,1:nlay,1:nq)=0 |
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| 222 | pdtcloud(1:ngrid,1:nlay)=0 |
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| 223 | |
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[358] | 224 | c Update the needed variables |
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| 225 | do l=1,nlay |
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| 226 | do ig=1,ngrid |
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| 227 | c Temperature |
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| 228 | zt(ig,l)=pt(ig,l)+ pdt(ig,l)*ptimestep |
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| 229 | c Dust mass mixing ratio |
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| 230 | zq(ig,l,igcm_dust_mass) = |
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| 231 | & pq(ig,l,igcm_dust_mass) + |
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| 232 | & pdq(ig,l,igcm_dust_mass) * ptimestep |
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| 233 | zq0(ig,l,igcm_dust_mass)=zq(ig,l,igcm_dust_mass) |
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| 234 | c Dust particle number |
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| 235 | zq(ig,l,igcm_dust_number) = |
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[411] | 236 | & pq(ig,l,igcm_dust_number) + |
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| 237 | & pdq(ig,l,igcm_dust_number) * ptimestep |
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[358] | 238 | zq0(ig,l,igcm_dust_number)=zq(ig,l,igcm_dust_number) |
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[411] | 239 | c Update rdust from last tendencies |
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| 240 | rdust(ig,l)= |
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| 241 | & CBRT(r3n_q*zq(ig,l,igcm_dust_mass)/ |
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| 242 | & max(zq(ig,l,igcm_dust_number),0.01)) |
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| 243 | rdust(ig,l)=min(max(rdust(ig,l),1.e-10),500.e-6) |
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[358] | 244 | c CCN mass mixing ratio |
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| 245 | zq(ig,l,igcm_ccn_mass)= |
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| 246 | & pq(ig,l,igcm_ccn_mass)+pdq(ig,l,igcm_ccn_mass)*ptimestep |
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| 247 | zq(ig,l,igcm_ccn_mass)=max(zq(ig,l,igcm_ccn_mass),1.E-30) |
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| 248 | zq0(ig,l,igcm_ccn_mass)=zq(ig,l,igcm_ccn_mass) |
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| 249 | c CCN particle number |
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| 250 | zq(ig,l,igcm_ccn_number)= |
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| 251 | & pq(ig,l,igcm_ccn_number)+pdq(ig,l,igcm_ccn_number)*ptimestep |
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| 252 | zq(ig,l,igcm_ccn_number)=max(zq(ig,l,igcm_ccn_number),1.E-30) |
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| 253 | zq0(ig,l,igcm_ccn_number)=zq(ig,l,igcm_ccn_number) |
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| 254 | c Water vapor |
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| 255 | zq(ig,l,igcm_h2o_vap)= |
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| 256 | & pq(ig,l,igcm_h2o_vap)+pdq(ig,l,igcm_h2o_vap)*ptimestep |
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| 257 | zq(ig,l,igcm_h2o_vap)=max(zq(ig,l,igcm_h2o_vap),1.E-30) ! FF 12/2004 |
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| 258 | zq0(ig,l,igcm_h2o_vap)=zq(ig,l,igcm_h2o_vap) |
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| 259 | c Water ice |
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| 260 | zq(ig,l,igcm_h2o_ice)= |
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| 261 | & pq(ig,l,igcm_h2o_ice)+pdq(ig,l,igcm_h2o_ice)*ptimestep |
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| 262 | zq(ig,l,igcm_h2o_ice)=max(zq(ig,l,igcm_h2o_ice),0.) ! FF 12/2004 |
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| 263 | zq0(ig,l,igcm_h2o_ice)=zq(ig,l,igcm_h2o_ice) |
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| 264 | enddo |
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| 265 | enddo |
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| 266 | |
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| 267 | c------------------------------------------------------------------ |
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| 268 | c Cloud microphysical scheme |
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| 269 | c------------------------------------------------------------------ |
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| 270 | |
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| 271 | Cste = ptimestep * 4. * pi * rho_ice |
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[541] | 272 | dev2 = 1. / ( sqrt(2.) * sigma_ice ) |
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[358] | 273 | |
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| 274 | call watersat(ngridmx*nlayermx,zt,pplay,zqsat) |
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| 275 | |
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[411] | 276 | count = 0 |
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[358] | 277 | |
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| 278 | c Main loop over the GCM's grid |
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| 279 | DO l=1,nlay |
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| 280 | DO ig=1,ngrid |
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| 281 | |
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| 282 | c Get the partial pressure of water vapor and its saturation ratio |
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| 283 | ph2o = zq(ig,l,igcm_h2o_vap) * (44./18.) * pplay(ig,l) |
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| 284 | satu = zq(ig,l,igcm_h2o_vap) / zqsat(ig,l) |
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[411] | 285 | |
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| 286 | IF ((satu .ge. 1)! ) THEN ! if we have condensation |
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[520] | 287 | & .or. ( zq(ig,l,igcm_ccn_number)*tauscaling(ig) |
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| 288 | & .ge. 2) ) THEN ! or sublimation |
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[358] | 289 | |
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[411] | 290 | |
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[358] | 291 | c Expand the dust moments into a binned distribution |
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[411] | 292 | Mo = zq(ig,l,igcm_dust_mass)* tauscaling(ig) |
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| 293 | No = zq(ig,l,igcm_dust_number)* tauscaling(ig)+ 1.e-30 |
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[358] | 294 | Rn = rdust(ig,l) |
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[530] | 295 | Rn = -dlog(Rn) |
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| 296 | Rm = Rn - 3. * sigma_ice*sigma_ice |
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[541] | 297 | yeahn = derf( (rb_cld(1)+Rn) *dev2) |
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| 298 | yeahm = derf( (rb_cld(1)+Rm) *dev2) |
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[358] | 299 | do i = 1, nbin_cld |
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[530] | 300 | n_aer(i) = -0.5 * No * yeahn !! this ith previously computed |
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| 301 | m_aer(i) = -0.5 * Mo * yeahm !! this ith previously computed |
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[541] | 302 | yeahn = derf( (rb_cld(i+1)+Rn) *dev2) |
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| 303 | yeahm = derf( (rb_cld(i+1)+Rm) *dev2) |
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[530] | 304 | n_aer(i) = n_aer(i) + 0.5 * No * yeahn |
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| 305 | m_aer(i) = m_aer(i) + 0.5 * Mo * yeahm |
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[358] | 306 | enddo |
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[530] | 307 | !!! MORE EFFICIENT COMPUTATIONALLY THAN |
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| 308 | ! Rn = rdust(ig,l) |
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| 309 | ! Rm = Rn * exp( 3. * sigma_ice**2. ) |
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| 310 | ! Rn = 1. / Rn |
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| 311 | ! Rm = 1. / Rm |
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| 312 | ! do i = 1, nbin_cld |
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| 313 | ! n_aer(i) = 0.5 * No * ( derf( dlog(rb_cld(i+1)*Rn) * dev2 ) |
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| 314 | ! & -derf( dlog(rb_cld(i) * Rn) * dev2 ) ) |
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| 315 | ! m_aer(i) = 0.5 * Mo * ( derf( dlog(rb_cld(i+1)*Rm) * dev2 ) |
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| 316 | ! & -derf( dlog(rb_cld(i) * Rm) * dev2 ) ) |
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| 317 | ! enddo |
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| 318 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
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| 319 | |
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[358] | 320 | ! sumcheck = 0 |
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| 321 | ! do i = 1, nbin_cld |
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| 322 | ! sumcheck = sumcheck + n_aer(i) |
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| 323 | ! enddo |
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| 324 | ! sumcheck = abs(sumcheck/No - 1) |
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| 325 | ! if ((sumcheck .gt. 1e-5).and. (1./Rn .gt. rmin_cld)) then |
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| 326 | ! print*, "WARNING, No sumcheck PROBLEM" |
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| 327 | ! print*, "sumcheck, No",sumcheck, No |
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| 328 | ! print*, "min radius, Rn, ig, l", rmin_cld, 1./Rn, ig, l |
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| 329 | ! print*, "Dust binned distribution", n_aer |
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| 330 | ! endif |
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| 331 | ! |
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| 332 | ! sumcheck = 0 |
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| 333 | ! do i = 1, nbin_cld |
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[411] | 334 | ! sumcheck = sumcheck + m_aer(i) |
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[358] | 335 | ! enddo |
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| 336 | ! sumcheck = abs(sumcheck/Mo - 1) |
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| 337 | ! if ((sumcheck .gt. 1e-5) .and. (1./Rn .gt. rmin_cld)) then |
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| 338 | ! print*, "WARNING, Mo sumcheck PROBLEM" |
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[411] | 339 | ! print*, "sumcheck, Mo",sumcheck, Mo |
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[358] | 340 | ! print*, "min radius, Rm, ig, l", rmin_cld, 1./Rm, ig, l |
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| 341 | ! print*, "Dust binned distribution", m_aer |
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| 342 | ! endif |
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| 343 | |
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| 344 | c Get the rates of nucleation |
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| 345 | call nuclea(ph2o,zt(ig,l),satu,n_aer,rate) |
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[411] | 346 | |
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[358] | 347 | |
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| 348 | dN = 0. |
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| 349 | dM = 0. |
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[455] | 350 | rate_out(ig,l) = 0 |
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[358] | 351 | do i = 1, nbin_cld |
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[520] | 352 | ! schema simple |
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[358] | 353 | n_aer(i) = n_aer(i) / ( 1. + rate(i)*ptimestep ) |
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| 354 | m_aer(i) = m_aer(i) / ( 1. + rate(i)*ptimestep ) |
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| 355 | dN = dN + n_aer(i) * rate(i) * ptimestep |
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| 356 | dM = dM + m_aer(i) * rate(i) * ptimestep |
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[520] | 357 | !rate_out(ig,l)=rate_out(ig,l)+rate(i) |
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[358] | 358 | enddo |
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| 359 | |
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| 360 | Mo = zq0(ig,l,igcm_h2o_ice) + |
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[411] | 361 | & zq0(ig,l,igcm_ccn_mass)* tauscaling(ig) + 1.e-30 |
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| 362 | No = zq0(ig,l,igcm_ccn_number)* tauscaling(ig)+ 1e-30 |
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[358] | 363 | !write(*,*) "l,cloud particles,cloud mass",l, No, Mo |
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| 364 | rhocloud(ig,l) = zq0(ig,l,igcm_h2o_ice) / Mo * rho_ice |
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[411] | 365 | & +zq0(ig,l,igcm_ccn_mass)* tauscaling(ig) |
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| 366 | & / Mo * rho_dust |
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[358] | 367 | rhocloud(ig,l) = min(max(rhocloud(ig,l),rho_ice),rho_dust) |
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[541] | 368 | if ((Mo.lt.1.e-20) .or. (No.le.1)) then |
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| 369 | rice(ig,l) = 1.e-8 |
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| 370 | else |
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| 371 | rice(ig,l) = |
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| 372 | & CBRT( real(Mo)/real(No) * 0.75 / pi / rhocloud(ig,l) ) !**(1./3.) |
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| 373 | endif |
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[411] | 374 | c nuice(ig,l)=nuice_ref ! used for rad. transfer calculations |
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[358] | 375 | seq = exp( 2.*sig(zt(ig,l))*mh2o / |
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| 376 | & (rho_ice*rgp*zt(ig,l)*rice(ig,l)) ) |
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| 377 | |
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| 378 | call growthrate(ptimestep,zt(ig,l),pplay(ig,l), |
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| 379 | & ph2o,ph2o/satu,seq,rice(ig,l),gr) |
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| 380 | |
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| 381 | up = Cste * gr * rice(ig,l) * No * seq + |
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| 382 | & zq(ig,l,igcm_h2o_vap) |
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| 383 | dwn = Cste * gr * rice(ig,l) * No / zqsat(ig,l)+ 1. |
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| 384 | |
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| 385 | Ctot = zq0(ig,l,igcm_h2o_ice) + zq(ig,l,igcm_h2o_vap) |
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| 386 | |
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| 387 | newvap = min(up/dwn,Ctot) |
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| 388 | |
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| 389 | gr = gr * ( newvap/zqsat(ig,l) - seq ) |
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| 390 | |
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| 391 | |
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| 392 | dMice = min( max(Cste * No * rice(ig,l) * gr, |
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| 393 | & -zq(ig,l,igcm_h2o_ice) ), |
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| 394 | & zq(ig,l,igcm_h2o_vap) ) |
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| 395 | |
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| 396 | c----------- TESTS 1D output --------- |
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[411] | 397 | satu_out(ig,l) = satu |
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[358] | 398 | Mcon_out(ig,l) = dMice |
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| 399 | newvap_out(ig,l) = newvap |
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| 400 | gr_out(ig,l) = gr |
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| 401 | dN_out(ig,l) = dN |
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| 402 | dM_out(ig,l) = dM |
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| 403 | c------------------------------------- |
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| 404 | |
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| 405 | c Water ice |
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| 406 | zq(ig,l,igcm_h2o_ice) = zq0(ig,l,igcm_h2o_ice) + |
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| 407 | & dMice |
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| 408 | |
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| 409 | c Water vapor |
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| 410 | zq(ig,l,igcm_h2o_vap) = zq0(ig,l,igcm_h2o_vap) - |
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| 411 | & dMice |
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[520] | 412 | |
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[358] | 413 | c If all the ice particles sublimate, all the condensation |
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| 414 | c nuclei are released: |
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| 415 | if (zq(ig,l,igcm_h2o_ice).le.1e-30) then |
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[411] | 416 | c for coherence |
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| 417 | dM = 0 |
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| 418 | dN = 0 |
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| 419 | dN_out(ig,l) = - zq(ig,l,igcm_ccn_number)*tauscaling(ig) |
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| 420 | dM_out(ig,l) = - zq(ig,l,igcm_ccn_mass)*tauscaling(ig) |
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[358] | 421 | c Water ice particles |
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| 422 | zq(ig,l,igcm_h2o_ice) = 0. |
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| 423 | c Dust particles |
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[411] | 424 | zq(ig,l,igcm_dust_mass) = zq(ig,l,igcm_dust_mass) + |
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| 425 | & zq(ig,l,igcm_ccn_mass) |
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| 426 | zq(ig,l,igcm_dust_number) = zq(ig,l,igcm_dust_number) + |
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| 427 | & zq(ig,l,igcm_ccn_number) |
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[358] | 428 | c CCNs |
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| 429 | zq(ig,l,igcm_ccn_mass) = 0. |
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| 430 | zq(ig,l,igcm_ccn_number) = 0. |
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| 431 | endif |
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| 432 | |
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[411] | 433 | dN = dN/ tauscaling(ig) |
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| 434 | dM = dM/ tauscaling(ig) |
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[358] | 435 | c Dust particles |
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[411] | 436 | zq(ig,l,igcm_dust_mass) = zq(ig,l,igcm_dust_mass) - dM |
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| 437 | zq(ig,l,igcm_dust_number) = zq(ig,l,igcm_dust_number) - dN |
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[358] | 438 | c CCNs |
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| 439 | zq(ig,l,igcm_ccn_mass) = zq(ig,l,igcm_ccn_mass) + dM |
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| 440 | zq(ig,l,igcm_ccn_number) = zq(ig,l,igcm_ccn_number) + dN |
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[520] | 441 | |
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| 442 | |
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[411] | 443 | pdqcloud(ig,l,igcm_dust_mass)=(zq(ig,l,igcm_dust_mass) |
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| 444 | & -zq0(ig,l,igcm_dust_mass))/ptimestep |
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| 445 | pdqcloud(ig,l,igcm_dust_number)=(zq(ig,l,igcm_dust_number) |
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| 446 | & -zq0(ig,l,igcm_dust_number))/ptimestep |
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| 447 | pdqcloud(ig,l,igcm_ccn_mass)=(zq(ig,l,igcm_ccn_mass) |
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| 448 | & -zq0(ig,l,igcm_ccn_mass))/ptimestep |
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| 449 | pdqcloud(ig,l,igcm_ccn_number)=(zq(ig,l,igcm_ccn_number) |
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| 450 | & -zq0(ig,l,igcm_ccn_number))/ptimestep |
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| 451 | pdqcloud(ig,l,igcm_h2o_vap)=(zq(ig,l,igcm_h2o_vap) |
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| 452 | & -zq0(ig,l,igcm_h2o_vap))/ptimestep |
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| 453 | pdqcloud(ig,l,igcm_h2o_ice)=(zq(ig,l,igcm_h2o_ice) |
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| 454 | & -zq0(ig,l,igcm_h2o_ice))/ptimestep |
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| 455 | |
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[520] | 456 | |
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[411] | 457 | count = count +1 |
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| 458 | ELSE ! for coherence (rdust, rice computations etc ..) |
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| 459 | zq(ig,l,igcm_dust_mass) = zq0(ig,l,igcm_dust_mass) |
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| 460 | zq(ig,l,igcm_dust_number) = zq0(ig,l,igcm_dust_number) |
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| 461 | zq(ig,l,igcm_ccn_mass) = zq0(ig,l,igcm_ccn_mass) |
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| 462 | zq(ig,l,igcm_ccn_number) = zq0(ig,l,igcm_ccn_number) |
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| 463 | zq(ig,l,igcm_h2o_ice) = zq0(ig,l,igcm_h2o_ice) |
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| 464 | zq(ig,l,igcm_h2o_vap) = zq0(ig,l,igcm_h2o_vap) |
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[358] | 465 | |
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[411] | 466 | ! pour les sorties de test |
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| 467 | satu_out(ig,l) = satu |
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| 468 | Mcon_out(ig,l) = 0 |
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[420] | 469 | newvap_out(ig,l) = zq(ig,l,igcm_h2o_vap) |
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| 470 | gr_out(ig,l) = 0 |
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| 471 | dN_out(ig,l) = 0 |
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| 472 | dM_out(ig,l) = 0 |
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[411] | 473 | |
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| 474 | ENDIF ! end if (saturation ratio > 1) or (there is h2o_ice) |
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| 475 | |
---|
| 476 | c-----update temperature |
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| 477 | lw=(2834.3-0.28*(zt(ig,l)-To)-0.004*(zt(ig,l)-To)**2)*1.e+3 |
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| 478 | pdtcloud(ig,l)=-pdqcloud(ig,l,igcm_h2o_vap)*lw/cpp |
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[520] | 479 | c pdtcloud(ig,l)=pdt(ig,l)-pdqcloud(ig,l,igcm_h2o_vap)*lw/cpp |
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[411] | 480 | |
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[520] | 481 | c----- update rice & rhocloud AFTER microphysic |
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[411] | 482 | Mo = zq(ig,l,igcm_h2o_ice) + |
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| 483 | & zq(ig,l,igcm_ccn_mass)* tauscaling(ig) + 1.e-30 |
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| 484 | No = zq(ig,l,igcm_ccn_number)* tauscaling(ig)+ 1e-30 |
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| 485 | rhocloud(ig,l) = zq(ig,l,igcm_h2o_ice) / Mo * rho_ice |
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| 486 | & +zq(ig,l,igcm_ccn_mass)* tauscaling(ig) |
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| 487 | & / Mo * rho_dust |
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| 488 | rhocloud(ig,l) = min(max(rhocloud(ig,l),rho_ice),rho_dust) |
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[520] | 489 | |
---|
| 490 | rice_out(ig,l)=rice(ig,l) |
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[541] | 491 | if ((Mo.lt.1.e-20) .or. (No.le.1)) then |
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| 492 | rice(ig,l) = 1.e-8 |
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| 493 | else |
---|
| 494 | rice(ig,l) = |
---|
| 495 | & CBRT( real(Mo)/real(No) * 0.75 / pi / rhocloud(ig,l) ) !**(1./3.) |
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| 496 | endif |
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[520] | 497 | rice_out(ig,l)=rice(ig,l)-rice_out(ig,l) |
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[411] | 498 | |
---|
| 499 | nuice(ig,l)=nuice_ref ! used for rad. transfer calculations |
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[358] | 500 | |
---|
[411] | 501 | c----- update rdust and sedimentation radius |
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[358] | 502 | rdust(ig,l)= |
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| 503 | & CBRT(r3n_q*zq(ig,l,igcm_dust_mass)/ |
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| 504 | & max(zq(ig,l,igcm_dust_number),0.01)) |
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| 505 | rdust(ig,l)=min(max(rdust(ig,l),1.e-10),500.e-6) |
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[411] | 506 | |
---|
[530] | 507 | rsedcloud(ig,l)=max( rice(ig,l)*(1.+nuice_sed)* |
---|
| 508 | & (1.+nuice_sed)*(1.+nuice_sed), |
---|
[358] | 509 | & rdust(ig,l) ) |
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| 510 | rsedcloud(ig,l)=min(rsedcloud(ig,l),1.e-4) |
---|
| 511 | |
---|
[411] | 512 | ENDDO |
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| 513 | ENDDO |
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[520] | 514 | |
---|
| 515 | ! print*, 'SATU' |
---|
| 516 | ! print*, satu_out(1,:) |
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[411] | 517 | |
---|
[358] | 518 | c------------------------------------------------------------------ |
---|
| 519 | c------------------------------------------------------------------ |
---|
| 520 | c------------------------------------------------------------------ |
---|
| 521 | c------------------------------------------------------------------ |
---|
[411] | 522 | c------------------------------------------------------------------ |
---|
| 523 | c TESTS |
---|
[420] | 524 | |
---|
| 525 | IF (output_sca) then |
---|
[411] | 526 | |
---|
| 527 | print*, 'count is ',count, ' i.e. ', |
---|
| 528 | & count*100/(nlay*ngrid), '% for microphys computation' |
---|
[358] | 529 | |
---|
[420] | 530 | dM_col(:) = 0 |
---|
| 531 | dN_col(:) = 0 |
---|
| 532 | Mdust_col(:) = 0 |
---|
| 533 | Ndust_col(:) = 0 |
---|
| 534 | Mccn_col(:) = 0 |
---|
| 535 | Nccn_col(:) = 0 |
---|
[520] | 536 | dMice_col(:) = 0 |
---|
| 537 | drice_col(:) = 0 |
---|
| 538 | icetot(:) = 0 |
---|
[420] | 539 | do l=1, nlay |
---|
| 540 | do ig=1,ngrid |
---|
| 541 | dM_col(ig) = dM_col(ig) + |
---|
| 542 | & dM_out(ig,l)*(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
| 543 | dN_col(ig) = dN_col(ig) + |
---|
| 544 | & dN_out(ig,l)*(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
| 545 | Mdust_col(ig) = Mdust_col(ig) + |
---|
| 546 | & zq(ig,l,igcm_dust_mass)*tauscaling(ig) |
---|
| 547 | & *(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
| 548 | Ndust_col(ig) = Ndust_col(ig) + |
---|
| 549 | & zq(ig,l,igcm_dust_number)*tauscaling(ig) |
---|
| 550 | & *(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
| 551 | Mccn_col(ig) = Mccn_col(ig) + |
---|
| 552 | & zq(ig,l,igcm_ccn_mass)*tauscaling(ig) |
---|
| 553 | & *(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
| 554 | Nccn_col(ig) = Nccn_col(ig) + |
---|
| 555 | & zq(ig,l,igcm_ccn_number)*tauscaling(ig) |
---|
| 556 | & *(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
[520] | 557 | dMice_col(ig) = dMice_col(ig) + |
---|
| 558 | & Mcon_out(ig,l) |
---|
| 559 | & *(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
| 560 | drice_col(ig) = drice_col(ig) + |
---|
| 561 | & rice_out(ig,l)*zq(ig,l,igcm_h2o_ice) |
---|
| 562 | & *(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
| 563 | icetot(ig) = icetot(ig) + |
---|
| 564 | & zq(ig,l,igcm_h2o_ice) |
---|
| 565 | & *(pplev(ig,l) - pplev(ig,l+1)) / g |
---|
[420] | 566 | enddo ! of do ig=1,ngrid |
---|
| 567 | enddo ! of do l=1,nlay |
---|
[520] | 568 | |
---|
| 569 | drice_col(ig) = drice_col(ig)/icetot(ig) |
---|
[358] | 570 | |
---|
[420] | 571 | IF (ngrid.ne.1) THEN ! 3D |
---|
[411] | 572 | call WRITEDIAGFI(ngrid,"satu","ratio saturation","",3, |
---|
| 573 | & satu_out) |
---|
| 574 | call WRITEDIAGFI(ngrid,"dM_col","dM column","kg",2, |
---|
| 575 | & dM_col) |
---|
| 576 | call WRITEDIAGFI(ngrid,"dN_col","dN column","N",2, |
---|
| 577 | & dN_col) |
---|
| 578 | call WRITEDIAGFI(ngrid,"Ndust_col","M column","N",2, |
---|
| 579 | & Ndust_col) |
---|
| 580 | call WRITEDIAGFI(ngrid,"Mdust_col","N column","kg",2, |
---|
| 581 | & Mdust_col) |
---|
| 582 | call WRITEDIAGFI(ngrid,"Nccn_col","M column","N",2, |
---|
| 583 | & Nccn_col) |
---|
| 584 | call WRITEDIAGFI(ngrid,"Mccn_col","N column","kg",2, |
---|
| 585 | & Mccn_col) |
---|
| 586 | call WRITEDIAGFI(ngrid,"dM","ccn variation","kg/kg",3, |
---|
| 587 | & dM_out) |
---|
| 588 | call WRITEDIAGFI(ngrid,"dN","ccn variation","#",3, |
---|
| 589 | & dN_out) |
---|
| 590 | ENDIF |
---|
[358] | 591 | |
---|
[411] | 592 | IF (ngrid.eq.1) THEN ! 1D |
---|
[358] | 593 | |
---|
| 594 | call WRITEDIAGFI(ngrid,"newvap","h2o newvap","kg",1, |
---|
| 595 | & newvap_out) |
---|
| 596 | call WRITEDIAGFI(ngrid,"growthrate","growth rate","m^2/s",1, |
---|
| 597 | & gr_out) |
---|
[455] | 598 | call WRITEDIAGFI(ngrid,"nuclearate","nucleation rate","",1, |
---|
| 599 | & rate_out) |
---|
[358] | 600 | call WRITEDIAGFI(ngrid,"dM","ccn variation","kg",1, |
---|
| 601 | & dM_out) |
---|
| 602 | call WRITEDIAGFI(ngrid,"dN","ccn variation","#",1, |
---|
| 603 | & dN_out) |
---|
[520] | 604 | call WRITEDIAGFI(ngrid,"dicetot","ice col var","kg/m2",0, |
---|
| 605 | & dMice_col) |
---|
| 606 | call WRITEDIAGFI(ngrid,"dricetot","ice col var","m",0, |
---|
| 607 | & drice_col) |
---|
[358] | 608 | call WRITEDIAGFI(ngrid,"mcond","h2o condensed mass","kg",1, |
---|
| 609 | & Mcon_out) |
---|
| 610 | call WRITEDIAGFI(ngrid,"zqsat","p vap sat","kg/kg",1, |
---|
| 611 | & zqsat) |
---|
| 612 | call WRITEDIAGFI(ngrid,"satu","ratio saturation","",1, |
---|
| 613 | & satu_out) |
---|
[411] | 614 | call WRITEDIAGFI(ngrid,"rice_sca","ice radius","m",1, |
---|
[358] | 615 | & rice) |
---|
[420] | 616 | call WRITEDIAGFI(ngrid,"rdust_sca","rdust","m",1, |
---|
[358] | 617 | & rdust) |
---|
| 618 | call WRITEDIAGFI(ngrid,"rsedcloud","rsedcloud","m",1, |
---|
| 619 | & rsedcloud) |
---|
| 620 | call WRITEDIAGFI(ngrid,"rhocloud","rhocloud","kg.m-3",1, |
---|
| 621 | & rhocloud) |
---|
[411] | 622 | call WRITEDIAGFI(ngrid,"dM_col","dM column","kg",0, |
---|
| 623 | & dM_col) |
---|
| 624 | call WRITEDIAGFI(ngrid,"dN_col","dN column","N",0, |
---|
| 625 | & dN_col) |
---|
| 626 | call WRITEDIAGFI(ngrid,"Ndust_col","M column","N",0, |
---|
| 627 | & Ndust_col) |
---|
| 628 | call WRITEDIAGFI(ngrid,"Mdust_col","N column","kg",0, |
---|
| 629 | & Mdust_col) |
---|
| 630 | call WRITEDIAGFI(ngrid,"Nccn_col","M column","N",0, |
---|
| 631 | & Nccn_col) |
---|
| 632 | call WRITEDIAGFI(ngrid,"Mccn_col","N column","kg",0, |
---|
| 633 | & Mccn_col) |
---|
[358] | 634 | ENDIF |
---|
[420] | 635 | ENDIF ! endif output_sca |
---|
[358] | 636 | c------------------------------------------------------------------ |
---|
| 637 | return |
---|
| 638 | end |
---|