[161] | 1 | ! |
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| 2 | ! $Id: calltherm.F90 1428 2010-09-13 08:43:37Z fairhead $ |
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| 3 | ! |
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[185] | 4 | subroutine calltherm_mars(dtime,zzlev,zzlay & |
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[161] | 5 | & ,pplay,paprs,pphi & |
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| 6 | & ,u_seri,v_seri,t_seri,pq_therm,q2_therm & |
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| 7 | & ,d_u_ajs,d_v_ajs,d_t_ajs,d_q_ajs,dq2_therm & |
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[185] | 8 | & ,fm_therm,entr_therm,detr_therm,lmax,zmax,& |
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[161] | 9 | & zw2,fraca,zpopsk,ztla,heatFlux,heatFlux_down,& |
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[173] | 10 | & buoyancyOut,buoyancyEst,hfmax,wmax) |
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[161] | 11 | |
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| 12 | USE ioipsl_getincom |
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| 13 | implicit none |
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| 14 | |
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[185] | 15 | #include "dimensions.h" |
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| 16 | #include "dimphys.h" |
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| 17 | |
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[161] | 18 | REAL dtime |
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[185] | 19 | LOGICAL logexpr0, logexpr2(ngridmx,nlayermx), logexpr1(ngridmx) |
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[161] | 20 | REAL fact |
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[185] | 21 | INTEGER nbptspb |
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[161] | 22 | |
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[185] | 23 | REAL, INTENT(IN) :: zzlay(ngridmx,nlayermx) |
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| 24 | REAL, INTENT(IN) :: zzlev(ngridmx,nlayermx+1) |
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[161] | 25 | |
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[185] | 26 | REAL u_seri(ngridmx,nlayermx),v_seri(ngridmx,nlayermx) |
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| 27 | REAL t_seri(ngridmx,nlayermx),pq_therm(ngridmx,nlayermx,nqmx) |
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| 28 | REAL q2_therm(ngridmx,nlayermx) |
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| 29 | REAL paprs(ngridmx,nlayermx+1) |
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| 30 | REAL pplay(ngridmx,nlayermx) |
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| 31 | REAL pphi(ngridmx,nlayermx) |
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| 32 | real zlev(ngridmx,nlayermx+1) |
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[161] | 33 | !test: on sort lentr et a* pour alimenter KE |
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[185] | 34 | REAL zw2(ngridmx,nlayermx+1),fraca(ngridmx,nlayermx+1) |
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| 35 | REAL zzw2(ngridmx,nlayermx+1) |
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[161] | 36 | |
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| 37 | !FH Update Thermiques |
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[185] | 38 | REAL d_t_ajs(ngridmx,nlayermx), d_q_ajs(ngridmx,nlayermx,nqmx) |
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| 39 | REAL d_u_ajs(ngridmx,nlayermx),d_v_ajs(ngridmx,nlayermx) |
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| 40 | REAL dq2_therm(ngridmx,nlayermx), dq2_the(ngridmx,nlayermx) |
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| 41 | real fm_therm(ngridmx,nlayermx+1) |
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| 42 | real entr_therm(ngridmx,nlayermx),detr_therm(ngridmx,nlayermx) |
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[161] | 43 | |
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| 44 | !******************************************************** |
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| 45 | ! declarations |
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[185] | 46 | real zpopsk(ngridmx,nlayermx) |
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| 47 | real ztla(ngridmx,nlayermx) |
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| 48 | real wmax(ngridmx) |
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| 49 | real hfmax(ngridmx) |
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| 50 | integer lmax(ngridmx) |
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| 51 | real zmax(ngridmx) |
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[161] | 52 | |
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| 53 | !nouvelles variables pour la convection |
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| 54 | !RC |
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| 55 | !on garde le zmax du pas de temps precedent |
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| 56 | !******************************************************** |
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| 57 | |
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| 58 | |
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| 59 | ! variables locales |
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[185] | 60 | REAL d_t_the(ngridmx,nlayermx), d_q_the(ngridmx,nlayermx,nqmx) |
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| 61 | REAL d_u_the(ngridmx,nlayermx),d_v_the(ngridmx,nlayermx) |
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[161] | 62 | ! |
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[185] | 63 | integer isplit,nsplit_thermals |
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| 64 | real r_aspect_thermals |
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[161] | 65 | |
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[185] | 66 | real zfm_therm(ngridmx,nlayermx+1),zdt |
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| 67 | real zentr_therm(ngridmx,nlayermx),zdetr_therm(ngridmx,nlayermx) |
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| 68 | real heatFlux(ngridmx,nlayermx) |
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| 69 | real heatFlux_down(ngridmx,nlayermx) |
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| 70 | real buoyancyOut(ngridmx,nlayermx) |
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| 71 | real buoyancyEst(ngridmx,nlayermx) |
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| 72 | real zheatFlux(ngridmx,nlayermx) |
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| 73 | real zheatFlux_down(ngridmx,nlayermx) |
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| 74 | real zbuoyancyOut(ngridmx,nlayermx) |
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| 75 | real zbuoyancyEst(ngridmx,nlayermx) |
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| 76 | |
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[161] | 77 | character (len=20) :: modname='calltherm' |
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| 78 | character (len=80) :: abort_message |
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| 79 | |
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| 80 | integer i,k |
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| 81 | logical, save :: first=.true. |
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| 82 | |
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[185] | 83 | REAL tstart,tstop |
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| 84 | |
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| 85 | |
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[161] | 86 | ! Modele du thermique |
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| 87 | ! =================== |
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[185] | 88 | |
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[276] | 89 | ! r_aspect_thermals ! ultimately conrols the amount of mass going through the thermals |
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[268] | 90 | ! decreasing it increases the thermals effect. Tests at gcm resolution |
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| 91 | ! shows that too low values destabilize the model |
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| 92 | ! when changing this value, one should check that the surface layer model |
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| 93 | ! outputs the correct Cd*u and Ch*u through changing the gustiness coefficient beta |
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[276] | 94 | |
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| 95 | |
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| 96 | #ifdef MESOSCALE |
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[277] | 97 | !! valid for timesteps < 200s |
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[276] | 98 | nsplit_thermals=2 |
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| 99 | r_aspect_thermals=0.7 |
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| 100 | #else |
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[284] | 101 | nsplit_thermals=50 |
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[276] | 102 | r_aspect_thermals=2. |
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| 103 | #endif |
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| 104 | |
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[161] | 105 | call getin("nsplit_thermals",nsplit_thermals) |
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| 106 | |
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| 107 | fm_therm(:,:)=0. |
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| 108 | detr_therm(:,:)=0. |
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| 109 | entr_therm(:,:)=0. |
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| 110 | |
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| 111 | heatFlux(:,:)=0. |
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| 112 | heatFlux_down(:,:)=0. |
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| 113 | buoyancyOut(:,:)=0. |
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| 114 | buoyancyEst(:,:)=0. |
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| 115 | |
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| 116 | zw2(:,:)=0. |
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| 117 | |
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| 118 | zdt=dtime/REAL(nsplit_thermals) |
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| 119 | |
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| 120 | do isplit=1,nsplit_thermals |
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| 121 | |
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[185] | 122 | ! call cpu_time(tstart) |
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| 123 | |
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| 124 | |
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[161] | 125 | ! On reinitialise les flux de masse a zero pour le cumul en |
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| 126 | ! cas de splitting |
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| 127 | |
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| 128 | zfm_therm(:,:)=0. |
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| 129 | zentr_therm(:,:)=0. |
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| 130 | zdetr_therm(:,:)=0. |
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| 131 | |
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| 132 | zheatFlux(:,:)=0. |
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| 133 | zheatFlux_down(:,:)=0. |
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| 134 | zbuoyancyOut(:,:)=0. |
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| 135 | zbuoyancyEst(:,:)=0. |
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| 136 | |
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| 137 | zzw2(:,:)=0. |
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| 138 | |
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| 139 | d_t_the(:,:)=0. |
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| 140 | d_u_the(:,:)=0. |
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| 141 | d_v_the(:,:)=0. |
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| 142 | dq2_the(:,:)=0. |
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[185] | 143 | if (nqmx .ne. 0) then |
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[161] | 144 | d_q_the(:,:,:)=0. |
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| 145 | endif |
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| 146 | |
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[185] | 147 | CALL thermcell_main_mars(zdt & |
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[161] | 148 | & ,pplay,paprs,pphi,zzlev,zzlay & |
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| 149 | & ,u_seri,v_seri,t_seri,pq_therm,q2_therm & |
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| 150 | & ,d_u_the,d_v_the,d_t_the,d_q_the,dq2_the & |
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[185] | 151 | & ,zfm_therm,zentr_therm,zdetr_therm,lmax,zmax & |
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[161] | 152 | & ,r_aspect_thermals & |
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| 153 | & ,zzw2,fraca,zpopsk & |
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| 154 | & ,ztla,zheatFlux,zheatFlux_down & |
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| 155 | & ,zbuoyancyOut,zbuoyancyEst) |
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| 156 | |
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| 157 | fact=1./REAL(nsplit_thermals) |
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| 158 | ! transformation de la derivee en tendance |
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| 159 | |
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| 160 | d_t_the(:,:)=d_t_the(:,:)*dtime*fact |
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| 161 | d_u_the(:,:)=d_u_the(:,:)*fact |
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| 162 | d_v_the(:,:)=d_v_the(:,:)*fact |
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| 163 | dq2_the(:,:)=dq2_the(:,:)*fact |
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| 164 | |
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[185] | 165 | if (nqmx .ne. 0) then |
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[161] | 166 | d_q_the(:,:,:)=d_q_the(:,:,:)*fact |
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| 167 | endif |
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| 168 | |
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| 169 | fm_therm(:,:)=fm_therm(:,:) & |
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| 170 | & +zfm_therm(:,:)*fact |
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| 171 | entr_therm(:,:)=entr_therm(:,:) & |
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| 172 | & +zentr_therm(:,:)*fact |
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| 173 | detr_therm(:,:)=detr_therm(:,:) & |
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| 174 | & +zdetr_therm(:,:)*fact |
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| 175 | |
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| 176 | heatFlux(:,:)=heatFlux(:,:) & |
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| 177 | & +zheatFlux(:,:)*fact |
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| 178 | heatFlux_down(:,:)=heatFlux_down(:,:) & |
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[173] | 179 | & +zheatFlux_down(:,:)*fact |
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[161] | 180 | buoyancyOut(:,:)=buoyancyOut(:,:) & |
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| 181 | & +zbuoyancyOut(:,:)*fact |
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| 182 | buoyancyEst(:,:)=buoyancyEst(:,:) & |
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[173] | 183 | & +zbuoyancyEst(:,:)*fact |
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[161] | 184 | |
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| 185 | zw2(:,:)=zw2(:,:) + zzw2(:,:)*fact |
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| 186 | |
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| 187 | ! accumulation de la tendance |
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| 188 | |
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| 189 | d_t_ajs(:,:)=d_t_ajs(:,:)+d_t_the(:,:) |
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| 190 | d_u_ajs(:,:)=d_u_ajs(:,:)+d_u_the(:,:) |
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| 191 | d_v_ajs(:,:)=d_v_ajs(:,:)+d_v_the(:,:) |
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| 192 | d_q_ajs(:,:,:)=d_q_ajs(:,:,:)+d_q_the(:,:,:) |
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| 193 | dq2_therm(:,:)=dq2_therm(:,:)+dq2_the(:,:) |
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| 194 | ! incrementation des variables meteo |
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| 195 | |
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| 196 | t_seri(:,:) = t_seri(:,:) + d_t_the(:,:) |
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| 197 | u_seri(:,:) = u_seri(:,:) + d_u_the(:,:) |
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| 198 | v_seri(:,:) = v_seri(:,:) + d_v_the(:,:) |
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| 199 | pq_therm(:,:,:) = pq_therm(:,:,:) + d_q_the(:,:,:) |
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| 200 | q2_therm(:,:) = q2_therm(:,:) + dq2_therm(:,:) |
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| 201 | |
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[185] | 202 | |
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| 203 | ! call cpu_time(tstop) |
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| 204 | ! print*,'elapsed time in thermals : ',tstop-tstart |
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| 205 | |
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[161] | 206 | enddo ! isplit |
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| 207 | |
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| 208 | |
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| 209 | !**************************************************************** |
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| 210 | |
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[185] | 211 | ! do i=1,ngridmx |
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| 212 | ! do k=1,nlayermx |
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[161] | 213 | ! if (ztla(i,k) .lt. 1.e-10) fraca(i,k) =0. |
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| 214 | ! print*,'youpi je sers a quelque chose !' |
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| 215 | ! enddo |
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| 216 | ! enddo |
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[173] | 217 | |
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[185] | 218 | DO i=1,ngridmx |
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[173] | 219 | hfmax(i)=MAXVAL(heatFlux(i,:)+heatFlux_down(i,:)) |
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| 220 | wmax(i)=MAXVAL(zw2(i,:)) |
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| 221 | ENDDO |
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| 222 | |
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[161] | 223 | return |
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| 224 | |
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| 225 | end |
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