[358] | 1 | subroutine simpleclouds(ngrid,nlay,ptimestep, |
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| 2 | & pplev,pplay,pzlev,pzlay,pt,pdt, |
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[520] | 3 | & pq,pdq,pdqcloud,pdtcloud, |
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[358] | 4 | & nq,tau,rice,nuice,rsedcloud) |
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| 5 | implicit none |
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| 6 | c------------------------------------------------------------------ |
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| 7 | c This routine is used to form clouds when a parcel of the GCM is |
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| 8 | c saturated. It is a simplified scheme, and there is almost no |
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| 9 | c microphysics involved. When the air is saturated, water-ice |
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| 10 | c clouds form on a fraction of the dust particles, specified by |
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| 11 | c the constant called "ccn_factor". There is no supersaturation, |
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| 12 | c and no nucleation rates computed. A more accurate scheme can |
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| 13 | c be found in the routine called "improvedclouds.F". |
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| 14 | |
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| 15 | c Modif de zq si saturation dans l'atmosphere |
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| 16 | c si zq(ig,l)> zqsat(ig,l) -> zq(ig,l)=zqsat(ig,l) |
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| 17 | c Le test est effectue de bas en haut. L'eau condensee |
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| 18 | c (si saturation) est remise dans la couche en dessous. |
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| 19 | c L'eau condensee dans la couche du bas est deposee a la surface |
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| 20 | |
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| 21 | c Authors: Franck Montmessin (water ice scheme) |
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| 22 | c Francois Forget (changed nuclei density & outputs) |
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| 23 | c Ehouarn Millour (sept.2008, tracers are now handled |
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| 24 | c by name and not fixed index) |
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| 25 | c J.-B. Madeleine (developed a single routine called |
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| 26 | c simpleclouds.F, and corrected calculations |
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| 27 | c of the typical CCN profile, Oct. 2011) |
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| 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 | c------------------------------------------------------------------ |
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| 37 | c Arguments: |
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| 38 | c --------- |
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| 39 | c Inputs: |
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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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| 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 pzlev(ngrid,nlay+1) ! altitude at layer boundaries |
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| 46 | REAL pzlay(ngrid,nlay) ! altitude at the middle of the layers |
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| 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 tau(ngridmx,naerkind) ! Column dust optical depth at each point |
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| 55 | |
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| 56 | c Output: |
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| 57 | REAL rice(ngrid,nlay) ! Ice mass mean radius (m) |
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| 58 | ! (r_c in montmessin_2004) |
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| 59 | REAL nuice(ngrid,nlay) ! Estimated effective variance |
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| 60 | ! of the size distribution |
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| 61 | real rsedcloud(ngridmx,nlayermx) ! Cloud sedimentation radius |
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| 62 | real pdqcloud(ngrid,nlay,nq) ! tendance de la condensation |
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| 63 | ! H2O(kg/kg.s-1) |
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| 64 | REAL pdtcloud(ngrid,nlay) ! tendance temperature due |
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| 65 | ! a la chaleur latente |
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| 66 | |
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| 67 | c------------------------------------------------------------------ |
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| 68 | c Local variables: |
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| 69 | |
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| 70 | LOGICAL firstcall |
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| 71 | DATA firstcall/.true./ |
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| 72 | SAVE firstcall |
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| 73 | |
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| 74 | REAL CBRT |
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| 75 | EXTERNAL CBRT |
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| 76 | |
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| 77 | INTEGER ig,l |
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| 78 | |
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| 79 | REAL zq(ngridmx,nlayermx,nqmx) ! local value of tracers |
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| 80 | REAL zq0(ngridmx,nlayermx,nqmx) ! local initial value of tracers |
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| 81 | REAL zt(ngridmx,nlayermx) ! local value of temperature |
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| 82 | REAL zqsat(ngridmx,nlayermx) ! saturation |
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| 83 | REAL*8 dzq ! masse de glace echangee (kg/kg) |
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| 84 | REAL lw !Latent heat of sublimation (J.kg-1) |
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| 85 | REAL,PARAMETER :: To=273.15 ! reference temperature, T=273.15 K |
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| 86 | real rdusttyp(ngridmx,nlayermx) ! Typical dust geom. mean radius (m) |
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| 87 | REAL ccntyp(ngridmx,nlayermx) |
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| 88 | ! Typical dust number density (#/kg) |
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| 89 | c CCN reduction factor |
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[420] | 90 | c REAL, PARAMETER :: ccn_factor = 4.5 !! comme TESTS_JB // 1. avant |
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[358] | 91 | |
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| 92 | REAL Mcon_out(ngridmx,nlayermx) ! mass to be condensed (not dMice !!) |
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| 93 | |
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| 94 | c----------------------------------------------------------------------- |
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| 95 | c 1. initialisation |
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| 96 | c ----------------- |
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| 97 | |
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| 98 | c On "update" la valeur de q(nqmx) (water vapor) et temperature. |
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| 99 | c On effectue qqes calculs preliminaires sur les couches : |
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| 100 | |
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| 101 | do l=1,nlay |
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| 102 | do ig=1,ngrid |
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| 103 | zq(ig,l,igcm_h2o_vap)= |
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| 104 | & pq(ig,l,igcm_h2o_vap)+pdq(ig,l,igcm_h2o_vap)*ptimestep |
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| 105 | zq(ig,l,igcm_h2o_vap)=max(zq(ig,l,igcm_h2o_vap),1.E-30) ! FF 12/2004 |
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| 106 | zq0(ig,l,igcm_h2o_vap)=zq(ig,l,igcm_h2o_vap) |
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| 107 | zt(ig,l)=pt(ig,l)+ pdt(ig,l)*ptimestep |
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| 108 | |
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| 109 | zq(ig,l,igcm_h2o_ice)= |
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| 110 | & pq(ig,l,igcm_h2o_ice)+pdq(ig,l,igcm_h2o_ice)*ptimestep |
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| 111 | zq(ig,l,igcm_h2o_ice)=max(zq(ig,l,igcm_h2o_ice),0.) ! FF 12/2004 |
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| 112 | zq0(ig,l,igcm_h2o_ice)=zq(ig,l,igcm_h2o_ice) |
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| 113 | enddo |
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| 114 | enddo |
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| 115 | |
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| 116 | do l=1,nlay |
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| 117 | do ig=1,ngrid |
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| 118 | |
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| 119 | c Typical dust radius profile: |
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| 120 | rdusttyp(ig,l)= max(.8e-6*exp(-pzlay(ig,l)/18000.),1.e-9) |
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| 121 | |
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| 122 | c Typical CCN profile: |
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| 123 | c Corrected equation, following Montmessin et al. 2004 |
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| 124 | c (N0=2e6 m-3 has been converted into N0=1.3e8 kg-1, otherwise |
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| 125 | c the equation for rice is not homogeneous...) |
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| 126 | ccntyp(ig,l)= |
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| 127 | & 1.3e+8*max(tau(ig,1),0.001)/0.1*exp(-pzlay(ig,l)/10000.) |
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| 128 | c The previously used profile was not correct: |
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| 129 | c ccntyp(ig,l)=( epaisseur(ig,l)/masse(ig,l) ) * |
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| 130 | c & 2.e+6/0.1*max(tau(ig,1),0.001)*exp(-pzlay(ig,l)/10000.) |
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| 131 | |
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| 132 | c Reduce number of nuclei |
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| 133 | ! TEMPORAIRE : decrease the number of CCNs FF 04/200 |
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| 134 | ! reduction facteur 3 |
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| 135 | ! ccntyp(ig,l) = ccntyp(ig,l) / 27. |
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| 136 | ! reduction facteur 2 |
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| 137 | ! ccntyp(ig,l) = ccntyp(ig,l) / 8. |
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| 138 | c ----------------------------------------------------------------- |
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| 139 | ccntyp(ig,l) = ccntyp(ig,l) / ccn_factor |
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| 140 | |
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| 141 | enddo ! of do ig=1,ngrid |
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[520] | 142 | enddo ! of do l=1,nlay |
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[358] | 143 | |
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| 144 | pdqcloud(1:ngrid,1:nlay,1:nq)=0 |
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| 145 | pdtcloud(1:ngrid,1:nlay)=0 |
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| 146 | |
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| 147 | c ---------------------------------------------- |
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| 148 | c |
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| 149 | c |
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| 150 | c Rapport de melange a saturation dans la couche l : ------- |
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| 151 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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| 152 | |
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| 153 | call watersat(ngridmx*nlayermx,zt,pplay,zqsat) |
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| 154 | |
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| 155 | c taux de condensation (kg/kg/s-1) dans les differentes couches |
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| 156 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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| 157 | |
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| 158 | do l=1,nlay |
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| 159 | do ig=1,ngrid |
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| 160 | |
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| 161 | if (zq(ig,l,igcm_h2o_vap).ge.zqsat(ig,l))then ! Condensation |
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| 162 | dzq=zq(ig,l,igcm_h2o_vap)-zqsat(ig,l) |
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| 163 | elseif(zq(ig,l,igcm_h2o_vap).lt.zqsat(ig,l))then ! Sublimation |
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| 164 | dzq=-min(zqsat(ig,l)-zq(ig,l,igcm_h2o_vap), |
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| 165 | & zq(ig,l,igcm_h2o_ice)) |
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| 166 | endif |
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| 167 | |
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| 168 | c Water Mass change |
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| 169 | c ~~~~~~~~~~~~~~~~~ |
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| 170 | zq(ig,l,igcm_h2o_ice)=zq(ig,l,igcm_h2o_ice)+dzq |
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| 171 | zq(ig,l,igcm_h2o_vap)=zq(ig,l,igcm_h2o_vap)-dzq |
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| 172 | |
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| 173 | Mcon_out(ig,l) = dzq |
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| 174 | |
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| 175 | c Calcul du rayon moyen des particules de glace. |
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| 176 | c Hypothese : Dans une couche, la glace presente se |
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| 177 | c repartit uniformement autour du nbre de poussieres |
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| 178 | c dont le rayon moyen est prescrit par rdusttyp. |
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| 179 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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| 180 | rice(ig,l)=max( CBRT ( (zq(ig,l,igcm_h2o_ice)/rho_ice |
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| 181 | & +ccntyp(ig,l)*(4./3.)*pi*rdusttyp(ig,l)**3.) |
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| 182 | & /(ccntyp(ig,l)*4./3.*pi) ), rdusttyp(ig,l)) |
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| 183 | c Effective variance of the size distribution |
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| 184 | nuice(ig,l)=nuice_ref |
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| 185 | |
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| 186 | c Sedimentation radius: |
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| 187 | c ~~~~~~~~~~~~~~~~~~~~ |
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| 188 | |
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| 189 | rsedcloud(ig,l)=max( rice(ig,l)*(1.+nuice_sed)**3., |
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| 190 | & rdusttyp(ig,l) ) |
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| 191 | rsedcloud(ig,l)=min(rsedcloud(ig,l),1.e-4) |
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| 192 | |
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| 193 | enddo ! of do ig=1,ngrid |
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| 194 | enddo ! of do l=1,nlay |
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| 195 | |
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| 196 | c Tendance finale |
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| 197 | c ~~~~~~~~~~~~~~~ |
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| 198 | do l=1, nlay |
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| 199 | do ig=1,ngridmx |
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| 200 | pdqcloud(ig,l,igcm_h2o_vap)=(zq(ig,l,igcm_h2o_vap) |
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| 201 | & -zq0(ig,l,igcm_h2o_vap))/ptimestep |
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| 202 | pdqcloud(ig,l,igcm_h2o_ice) = |
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| 203 | & (zq(ig,l,igcm_h2o_ice) - zq0(ig,l,igcm_h2o_ice))/ptimestep |
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| 204 | lw=(2834.3-0.28*(zt(ig,l)-To)-0.004*(zt(ig,l)-To)**2)*1.e+3 |
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| 205 | pdtcloud(ig,l)=-pdqcloud(ig,l,igcm_h2o_vap)*lw/cpp |
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| 206 | end do |
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| 207 | end do |
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| 208 | |
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| 209 | c------------------------------------------------------------------ |
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| 210 | c TEST_JBM |
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[520] | 211 | ! IF (ngrid.eq.1) THEN |
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| 212 | ! call WRITEDIAGFI(ngrid,"mcond","h2o condensed mass","kg",1, |
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| 213 | ! & Mcon_out) |
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| 214 | ! call WRITEDIAGFI(ngrid,"rdusttyp","rdusttyp","m",1, |
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| 215 | ! & rdusttyp) |
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| 216 | ! call WRITEDIAGFI(ngrid,"ccntyp","ccntyp","kg-1",1, |
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| 217 | ! & ccntyp) |
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| 218 | ! ENDIF |
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[358] | 219 | c------------------------------------------------------------------ |
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| 220 | return |
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| 221 | end |
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