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