[1969] | 1 | MODULE vdifc_mod |
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| 2 | |
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| 3 | IMPLICIT NONE |
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| 4 | |
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| 5 | CONTAINS |
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| 6 | |
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[38] | 7 | SUBROUTINE vdifc(ngrid,nlay,nq,co2ice,ppopsk, |
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| 8 | $ ptimestep,pcapcal,lecrit, |
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| 9 | $ pplay,pplev,pzlay,pzlev,pz0, |
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| 10 | $ pu,pv,ph,pq,ptsrf,pemis,pqsurf, |
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| 11 | $ pdufi,pdvfi,pdhfi,pdqfi,pfluxsrf, |
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| 12 | $ pdudif,pdvdif,pdhdif,pdtsrf,pq2, |
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[660] | 13 | $ pdqdif,pdqsdif,wstar,zcdv_true,zcdh_true, |
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[1996] | 14 | $ hfmax,pcondicea_co2microp,sensibFlux, |
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[2260] | 15 | $ dustliftday,local_time,watercap, dwatercap_dif) |
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[1236] | 16 | |
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[1036] | 17 | use tracer_mod, only: noms, igcm_dust_mass, igcm_dust_number, |
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| 18 | & igcm_dust_submicron, igcm_h2o_vap, |
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[1974] | 19 | & igcm_h2o_ice, alpha_lift, |
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[2312] | 20 | & igcm_hdo_vap, igcm_hdo_ice, |
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[1974] | 21 | & igcm_stormdust_mass, igcm_stormdust_number |
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[1224] | 22 | use surfdat_h, only: watercaptag, frost_albedo_threshold, dryness |
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[1969] | 23 | USE comcstfi_h, ONLY: cpp, r, rcp, g |
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[1996] | 24 | use watersat_mod, only: watersat |
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[1242] | 25 | use turb_mod, only: turb_resolved, ustar, tstar |
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[2160] | 26 | use compute_dtau_mod, only: ti_injection_sol,tf_injection_sol |
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[2312] | 27 | use hdo_surfex_mod, only: hdo_surfex |
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[2409] | 28 | use dust_param_mod, only: doubleq, submicron, lifting |
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[2312] | 29 | |
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[38] | 30 | IMPLICIT NONE |
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| 31 | |
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| 32 | c======================================================================= |
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| 33 | c |
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| 34 | c subject: |
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| 35 | c -------- |
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| 36 | c Turbulent diffusion (mixing) for potential T, U, V and tracer |
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| 37 | c |
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| 38 | c Shema implicite |
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| 39 | c On commence par rajouter au variables x la tendance physique |
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| 40 | c et on resoult en fait: |
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| 41 | c x(t+1) = x(t) + dt * (dx/dt)phys(t) + dt * (dx/dt)difv(t+1) |
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| 42 | c |
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| 43 | c author: |
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| 44 | c ------ |
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| 45 | c Hourdin/Forget/Fournier |
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| 46 | c======================================================================= |
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| 47 | |
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| 48 | c----------------------------------------------------------------------- |
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| 49 | c declarations: |
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| 50 | c ------------- |
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| 51 | |
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[1944] | 52 | include "callkeys.h" |
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| 53 | include "microphys.h" |
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[38] | 54 | |
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| 55 | c |
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| 56 | c arguments: |
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| 57 | c ---------- |
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| 58 | |
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[1036] | 59 | INTEGER,INTENT(IN) :: ngrid,nlay |
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| 60 | REAL,INTENT(IN) :: ptimestep |
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| 61 | REAL,INTENT(IN) :: pplay(ngrid,nlay),pplev(ngrid,nlay+1) |
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| 62 | REAL,INTENT(IN) :: pzlay(ngrid,nlay),pzlev(ngrid,nlay+1) |
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| 63 | REAL,INTENT(IN) :: pu(ngrid,nlay),pv(ngrid,nlay) |
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| 64 | REAL,INTENT(IN) :: ph(ngrid,nlay) |
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| 65 | REAL,INTENT(IN) :: ptsrf(ngrid),pemis(ngrid) |
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| 66 | REAL,INTENT(IN) :: pdufi(ngrid,nlay),pdvfi(ngrid,nlay) |
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| 67 | REAL,INTENT(IN) :: pdhfi(ngrid,nlay) |
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| 68 | REAL,INTENT(IN) :: pfluxsrf(ngrid) |
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| 69 | REAL,INTENT(OUT) :: pdudif(ngrid,nlay),pdvdif(ngrid,nlay) |
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| 70 | REAL,INTENT(OUT) :: pdtsrf(ngrid),pdhdif(ngrid,nlay) |
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[1130] | 71 | REAL,INTENT(IN) :: pcapcal(ngrid) |
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| 72 | REAL,INTENT(INOUT) :: pq2(ngrid,nlay+1) |
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[38] | 73 | |
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| 74 | c Argument added for condensation: |
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[1036] | 75 | REAL,INTENT(IN) :: co2ice (ngrid), ppopsk(ngrid,nlay) |
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| 76 | logical,INTENT(IN) :: lecrit |
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[1996] | 77 | REAL,INTENT(IN) :: pcondicea_co2microp(ngrid,nlay)! tendency due to CO2 condensation (kg/kg.s-1) |
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| 78 | |
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[1036] | 79 | REAL,INTENT(IN) :: pz0(ngrid) ! surface roughness length (m) |
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[224] | 80 | |
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[256] | 81 | c Argument added to account for subgrid gustiness : |
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| 82 | |
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[1944] | 83 | REAL,INTENT(IN) :: wstar(ngrid), hfmax(ngrid)!, zi(ngrid) |
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[256] | 84 | |
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[38] | 85 | c Traceurs : |
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[1036] | 86 | integer,intent(in) :: nq |
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| 87 | REAL,INTENT(IN) :: pqsurf(ngrid,nq) |
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| 88 | real,intent(in) :: pq(ngrid,nlay,nq), pdqfi(ngrid,nlay,nq) |
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| 89 | real,intent(out) :: pdqdif(ngrid,nlay,nq) |
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[1974] | 90 | real,intent(out) :: pdqsdif(ngrid,nq) |
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| 91 | REAL,INTENT(in) :: dustliftday(ngrid) |
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| 92 | REAL,INTENT(in) :: local_time(ngrid) |
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[38] | 93 | |
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| 94 | c local: |
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| 95 | c ------ |
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| 96 | |
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[1130] | 97 | REAL :: pt(ngrid,nlay) |
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[473] | 98 | |
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[38] | 99 | INTEGER ilev,ig,ilay,nlev |
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| 100 | |
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[1047] | 101 | REAL z4st,zdplanck(ngrid) |
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| 102 | REAL zkv(ngrid,nlay+1),zkh(ngrid,nlay+1) |
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| 103 | REAL zkq(ngrid,nlay+1) |
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| 104 | REAL zcdv(ngrid),zcdh(ngrid) |
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| 105 | REAL zcdv_true(ngrid),zcdh_true(ngrid) ! drag coeff are used by the LES to recompute u* and hfx |
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| 106 | REAL zu(ngrid,nlay),zv(ngrid,nlay) |
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| 107 | REAL zh(ngrid,nlay) |
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| 108 | REAL ztsrf2(ngrid) |
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| 109 | REAL z1(ngrid),z2(ngrid) |
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| 110 | REAL za(ngrid,nlay),zb(ngrid,nlay) |
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| 111 | REAL zb0(ngrid,nlay) |
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| 112 | REAL zc(ngrid,nlay),zd(ngrid,nlay) |
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[38] | 113 | REAL zcst1 |
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[1047] | 114 | REAL zu2(ngrid) |
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[38] | 115 | |
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| 116 | EXTERNAL SSUM,SCOPY |
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| 117 | REAL SSUM |
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[1036] | 118 | LOGICAL,SAVE :: firstcall=.true. |
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[38] | 119 | |
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[626] | 120 | |
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[38] | 121 | c variable added for CO2 condensation: |
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| 122 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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[1047] | 123 | REAL hh , zhcond(ngrid,nlay) |
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| 124 | REAL,PARAMETER :: latcond=5.9e5 |
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| 125 | REAL,PARAMETER :: tcond1mb=136.27 |
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| 126 | REAL,SAVE :: acond,bcond |
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[669] | 127 | |
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[2179] | 128 | c For latent heat release from ground water ice sublimation |
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| 129 | REAL tsrf_lh(ngrid) ! temporary surface temperature |
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| 130 | REAL lh ! latent heat, formulation given in the Technical Document: |
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| 131 | ! "Modeling water ice sublimation under Phoenix-like conditions", Montmessin et al. 2004 |
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[1047] | 132 | ! REAL tsrf_lw(ngrid) |
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[1036] | 133 | ! REAL alpha |
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[2179] | 134 | ! REAL T1,T2 |
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| 135 | ! SAVE T1,T2 |
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| 136 | ! DATA T1,T2/-604.3,1080.7/ ! zeros of latent heat equation for ice |
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[38] | 137 | |
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| 138 | c Tracers : |
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| 139 | c ~~~~~~~ |
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| 140 | INTEGER iq |
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[1047] | 141 | REAL zq(ngrid,nlay,nq) |
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| 142 | REAL zq1temp(ngrid) |
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| 143 | REAL rho(ngrid) ! near surface air density |
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| 144 | REAL qsat(ngrid) |
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[38] | 145 | |
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[2312] | 146 | REAL hdoflux(ngrid) ! value of vapour flux of HDO |
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| 147 | REAL h2oflux(ngrid) ! value of vapour flux of H2O |
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| 148 | REAL old_h2o_vap(ngrid) ! traceur d'eau avant traitement |
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| 149 | |
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[38] | 150 | REAL kmixmin |
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| 151 | |
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[2260] | 152 | c Argument added for surface water ice budget: |
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| 153 | REAL,INTENT(IN) :: watercap(ngrid) |
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| 154 | REAL,INTENT(OUT) :: dwatercap_dif(ngrid) |
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| 155 | |
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[473] | 156 | c Mass-variation scheme : |
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| 157 | c ~~~~~~~ |
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| 158 | |
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| 159 | INTEGER j,l |
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[1047] | 160 | REAL zcondicea(ngrid,nlay) |
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| 161 | REAL zt(ngrid,nlay),ztcond(ngrid,nlay+1) |
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| 162 | REAL betam(ngrid,nlay),dmice(ngrid,nlay) |
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| 163 | REAL pdtc(ngrid,nlay) |
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| 164 | REAL zhs(ngrid,nlay) |
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| 165 | REAL,SAVE :: ccond |
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[473] | 166 | |
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| 167 | c Theta_m formulation for mass-variation scheme : |
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| 168 | c ~~~~~~~ |
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| 169 | |
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[1047] | 170 | INTEGER,SAVE :: ico2 |
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| 171 | INTEGER llnt(ngrid) |
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| 172 | REAL,SAVE :: m_co2, m_noco2, A , B |
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| 173 | REAL vmr_co2(ngrid,nlay) |
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[473] | 174 | REAL qco2,mmean |
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| 175 | |
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[1047] | 176 | REAL,INTENT(OUT) :: sensibFlux(ngrid) |
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[660] | 177 | |
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[2312] | 178 | !!MARGAUX |
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| 179 | REAL DoH_vap(ngrid,nlay) |
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| 180 | |
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[38] | 181 | c ** un petit test de coherence |
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| 182 | c -------------------------- |
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| 183 | |
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[1779] | 184 | ! AS: OK firstcall absolute |
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[38] | 185 | IF (firstcall) THEN |
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| 186 | c To compute: Tcond= 1./(bcond-acond*log(.0095*p)) (p in pascal) |
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| 187 | bcond=1./tcond1mb |
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| 188 | acond=r/latcond |
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[473] | 189 | ccond=cpp/(g*latcond) |
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[38] | 190 | PRINT*,'In vdifc: Tcond(P=1mb)=',tcond1mb,' Lcond=',latcond |
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[473] | 191 | PRINT*,' acond,bcond,ccond',acond,bcond,ccond |
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[38] | 192 | |
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[473] | 193 | |
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| 194 | ico2=0 |
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| 195 | |
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| 196 | if (tracer) then |
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| 197 | c Prepare Special treatment if one of the tracer is CO2 gas |
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[1036] | 198 | do iq=1,nq |
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[473] | 199 | if (noms(iq).eq."co2") then |
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| 200 | ico2=iq |
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| 201 | m_co2 = 44.01E-3 ! CO2 molecular mass (kg/mol) |
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| 202 | m_noco2 = 33.37E-3 ! Non condensible mol mass (kg/mol) |
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| 203 | c Compute A and B coefficient use to compute |
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| 204 | c mean molecular mass Mair defined by |
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| 205 | c 1/Mair = q(ico2)/m_co2 + (1-q(ico2))/m_noco2 |
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| 206 | c 1/Mair = A*q(ico2) + B |
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| 207 | A =(1/m_co2 - 1/m_noco2) |
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| 208 | B=1/m_noco2 |
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| 209 | endif |
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| 210 | enddo |
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| 211 | end if |
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| 212 | |
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[38] | 213 | firstcall=.false. |
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| 214 | ENDIF |
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| 215 | |
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| 216 | |
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| 217 | c----------------------------------------------------------------------- |
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| 218 | c 1. initialisation |
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| 219 | c ----------------- |
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| 220 | |
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| 221 | nlev=nlay+1 |
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| 222 | |
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[1035] | 223 | ! initialize output tendencies to zero: |
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| 224 | pdudif(1:ngrid,1:nlay)=0 |
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| 225 | pdvdif(1:ngrid,1:nlay)=0 |
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| 226 | pdhdif(1:ngrid,1:nlay)=0 |
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| 227 | pdtsrf(1:ngrid)=0 |
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| 228 | pdqdif(1:ngrid,1:nlay,1:nq)=0 |
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| 229 | pdqsdif(1:ngrid,1:nq)=0 |
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[2260] | 230 | dwatercap_dif(1:ngrid)=0 |
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[1035] | 231 | |
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[38] | 232 | c ** calcul de rho*dz et dt*rho/dz=dt*rho**2 g/dp |
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| 233 | c avec rho=p/RT=p/ (R Theta) (p/ps)**kappa |
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| 234 | c ---------------------------------------- |
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| 235 | |
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| 236 | DO ilay=1,nlay |
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| 237 | DO ig=1,ngrid |
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| 238 | za(ig,ilay)=(pplev(ig,ilay)-pplev(ig,ilay+1))/g |
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[473] | 239 | ! Mass variation scheme: |
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| 240 | betam(ig,ilay)=-za(ig,ilay)*latcond/(cpp*ppopsk(ig,ilay)) |
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[38] | 241 | ENDDO |
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| 242 | ENDDO |
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| 243 | |
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| 244 | zcst1=4.*g*ptimestep/(r*r) |
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| 245 | DO ilev=2,nlev-1 |
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| 246 | DO ig=1,ngrid |
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| 247 | zb0(ig,ilev)=pplev(ig,ilev)* |
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| 248 | s (pplev(ig,1)/pplev(ig,ilev))**rcp / |
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| 249 | s (ph(ig,ilev-1)+ph(ig,ilev)) |
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| 250 | zb0(ig,ilev)=zcst1*zb0(ig,ilev)*zb0(ig,ilev)/ |
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| 251 | s (pplay(ig,ilev-1)-pplay(ig,ilev)) |
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| 252 | ENDDO |
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| 253 | ENDDO |
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| 254 | DO ig=1,ngrid |
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[473] | 255 | zb0(ig,1)=ptimestep*pplev(ig,1)/(r*ptsrf(ig)) |
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[38] | 256 | ENDDO |
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| 257 | |
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| 258 | c ** diagnostique pour l'initialisation |
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| 259 | c ---------------------------------- |
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| 260 | |
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| 261 | IF(lecrit) THEN |
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| 262 | ig=ngrid/2+1 |
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| 263 | PRINT*,'Pression (mbar) ,altitude (km),u,v,theta, rho dz' |
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| 264 | DO ilay=1,nlay |
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| 265 | WRITE(*,'(6f11.5)') |
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| 266 | s .01*pplay(ig,ilay),.001*pzlay(ig,ilay), |
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| 267 | s pu(ig,ilay),pv(ig,ilay),ph(ig,ilay),za(ig,ilay) |
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| 268 | ENDDO |
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| 269 | PRINT*,'Pression (mbar) ,altitude (km),zb' |
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| 270 | DO ilev=1,nlay |
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| 271 | WRITE(*,'(3f15.7)') |
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| 272 | s .01*pplev(ig,ilev),.001*pzlev(ig,ilev), |
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| 273 | s zb0(ig,ilev) |
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| 274 | ENDDO |
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| 275 | ENDIF |
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| 276 | |
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[473] | 277 | c ----------------------------------- |
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[38] | 278 | c Potential Condensation temperature: |
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| 279 | c ----------------------------------- |
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| 280 | |
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[473] | 281 | c Compute CO2 Volume mixing ratio |
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| 282 | c ------------------------------- |
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| 283 | if (callcond.and.(ico2.ne.0)) then |
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| 284 | DO ilev=1,nlay |
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| 285 | DO ig=1,ngrid |
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[529] | 286 | qco2=MAX(1.E-30 |
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| 287 | & ,pq(ig,ilev,ico2)+pdqfi(ig,ilev,ico2)*ptimestep) |
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[473] | 288 | c Mean air molecular mass = 1/(q(ico2)/m_co2 + (1-q(ico2))/m_noco2) |
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| 289 | mmean=1/(A*qco2 +B) |
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| 290 | vmr_co2(ig,ilev) = qco2*mmean/m_co2 |
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| 291 | ENDDO |
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| 292 | ENDDO |
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| 293 | else |
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| 294 | DO ilev=1,nlay |
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| 295 | DO ig=1,ngrid |
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| 296 | vmr_co2(ig,ilev)=0.95 |
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| 297 | ENDDO |
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| 298 | ENDDO |
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| 299 | end if |
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[38] | 300 | |
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[473] | 301 | c forecast of atmospheric temperature zt and frost temperature ztcond |
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| 302 | c -------------------------------------------------------------------- |
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[38] | 303 | |
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[473] | 304 | if (callcond) then |
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| 305 | DO ilev=1,nlay |
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| 306 | DO ig=1,ngrid |
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[884] | 307 | ztcond(ig,ilev)= |
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| 308 | & 1./(bcond-acond*log(.01*vmr_co2(ig,ilev)*pplay(ig,ilev))) |
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| 309 | if (pplay(ig,ilev).lt.1e-4) ztcond(ig,ilev)=0.0 !mars Monica |
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[473] | 310 | ! zhcond(ig,ilev) = |
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| 311 | ! & (1./(bcond-acond*log(.0095*pplay(ig,ilev))))/ppopsk(ig,ilev) |
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| 312 | zhcond(ig,ilev) = ztcond(ig,ilev)/ppopsk(ig,ilev) |
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| 313 | END DO |
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| 314 | END DO |
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[884] | 315 | ztcond(:,nlay+1)=ztcond(:,nlay) |
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[473] | 316 | else |
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[884] | 317 | zhcond(:,:) = 0 |
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| 318 | ztcond(:,:) = 0 |
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[473] | 319 | end if |
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| 320 | |
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| 321 | |
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[38] | 322 | c----------------------------------------------------------------------- |
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| 323 | c 2. ajout des tendances physiques |
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| 324 | c ----------------------------- |
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| 325 | |
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| 326 | DO ilev=1,nlay |
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| 327 | DO ig=1,ngrid |
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| 328 | zu(ig,ilev)=pu(ig,ilev)+pdufi(ig,ilev)*ptimestep |
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| 329 | zv(ig,ilev)=pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep |
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| 330 | zh(ig,ilev)=ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
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[473] | 331 | ! zh(ig,ilev)=max(zh(ig,ilev),zhcond(ig,ilev)) |
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[38] | 332 | ENDDO |
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| 333 | ENDDO |
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| 334 | if(tracer) then |
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| 335 | DO iq =1, nq |
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| 336 | DO ilev=1,nlay |
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| 337 | DO ig=1,ngrid |
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| 338 | zq(ig,ilev,iq)=pq(ig,ilev,iq)+pdqfi(ig,ilev,iq)*ptimestep |
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| 339 | ENDDO |
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| 340 | ENDDO |
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| 341 | ENDDO |
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| 342 | end if |
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| 343 | |
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| 344 | c----------------------------------------------------------------------- |
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| 345 | c 3. schema de turbulence |
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| 346 | c -------------------- |
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| 347 | |
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| 348 | c ** source d'energie cinetique turbulente a la surface |
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| 349 | c (condition aux limites du schema de diffusion turbulente |
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| 350 | c dans la couche limite |
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| 351 | c --------------------- |
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| 352 | |
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[499] | 353 | CALL vdif_cd(ngrid,nlay,pz0,g,pzlay,pu,pv,wstar,ptsrf,ph |
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[1236] | 354 | & ,zcdv_true,zcdh_true) |
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[256] | 355 | |
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[290] | 356 | zu2(:)=pu(:,1)*pu(:,1)+pv(:,1)*pv(:,1) |
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[256] | 357 | |
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[291] | 358 | IF (callrichsl) THEN |
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[545] | 359 | zcdv(:)=zcdv_true(:)*sqrt(zu2(:)+ |
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| 360 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
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| 361 | zcdh(:)=zcdh_true(:)*sqrt(zu2(:)+ |
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| 362 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
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[496] | 363 | |
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[1242] | 364 | ustar(:)=sqrt(zcdv_true(:))*sqrt(zu2(:)+ |
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[545] | 365 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
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| 366 | |
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[1242] | 367 | tstar(:)=0. |
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[545] | 368 | DO ig=1,ngrid |
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| 369 | IF (zcdh_true(ig) .ne. 0.) THEN ! When Cd=Ch=0, u*=t*=0 |
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[1242] | 370 | tstar(ig)=(ph(ig,1)-ptsrf(ig))*zcdh(ig)/ustar(ig) |
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[545] | 371 | ENDIF |
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| 372 | ENDDO |
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| 373 | |
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[284] | 374 | ELSE |
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[545] | 375 | zcdv(:)=zcdv_true(:)*sqrt(zu2(:)) ! 1 / bulk aerodynamic momentum conductance |
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| 376 | zcdh(:)=zcdh_true(:)*sqrt(zu2(:)) ! 1 / bulk aerodynamic heat conductance |
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[1242] | 377 | ustar(:)=sqrt(zcdv_true(:))*sqrt(zu2(:)) |
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| 378 | tstar(:)=(ph(:,1)-ptsrf(:))*zcdh_true(:)/sqrt(zcdv_true(:)) |
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[290] | 379 | ENDIF |
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[38] | 380 | |
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[529] | 381 | ! Some usefull diagnostics for the new surface layer parametrization : |
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[290] | 382 | |
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[1130] | 383 | ! call WRITEDIAGFI(ngrid,'vdifc_zcdv_true', |
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[256] | 384 | ! & 'momentum drag','no units', |
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| 385 | ! & 2,zcdv_true) |
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[1130] | 386 | ! call WRITEDIAGFI(ngrid,'vdifc_zcdh_true', |
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[256] | 387 | ! & 'heat drag','no units', |
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| 388 | ! & 2,zcdh_true) |
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[1130] | 389 | ! call WRITEDIAGFI(ngrid,'vdifc_ust', |
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[473] | 390 | ! & 'friction velocity','m/s',2,ust) |
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[1130] | 391 | ! call WRITEDIAGFI(ngrid,'vdifc_tst', |
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[473] | 392 | ! & 'friction temperature','K',2,tst) |
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[1130] | 393 | ! call WRITEDIAGFI(ngrid,'vdifc_zcdv', |
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[268] | 394 | ! & 'aerodyn momentum conductance','m/s', |
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[256] | 395 | ! & 2,zcdv) |
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[1130] | 396 | ! call WRITEDIAGFI(ngrid,'vdifc_zcdh', |
---|
[268] | 397 | ! & 'aerodyn heat conductance','m/s', |
---|
[256] | 398 | ! & 2,zcdh) |
---|
| 399 | |
---|
[38] | 400 | c ** schema de diffusion turbulente dans la couche limite |
---|
| 401 | c ---------------------------------------------------- |
---|
[1240] | 402 | IF (.not. callyamada4) THEN |
---|
[529] | 403 | |
---|
[1130] | 404 | CALL vdif_kc(ngrid,nlay,nq,ptimestep,g,pzlev,pzlay |
---|
[38] | 405 | & ,pu,pv,ph,zcdv_true |
---|
[325] | 406 | & ,pq2,zkv,zkh,zq) |
---|
[529] | 407 | |
---|
[544] | 408 | ELSE |
---|
[38] | 409 | |
---|
[555] | 410 | pt(:,:)=ph(:,:)*ppopsk(:,:) |
---|
[1036] | 411 | CALL yamada4(ngrid,nlay,nq,ptimestep,g,r,pplev,pt |
---|
[1242] | 412 | s ,pzlev,pzlay,pu,pv,ph,pq,zcdv_true,pq2,zkv,zkh,zkq,ustar |
---|
[652] | 413 | s ,9) |
---|
[544] | 414 | ENDIF |
---|
| 415 | |
---|
[38] | 416 | if ((doubleq).and.(ngrid.eq.1)) then |
---|
| 417 | kmixmin = 80. !80.! minimum eddy mix coeff in 1D |
---|
| 418 | do ilev=1,nlay |
---|
| 419 | do ig=1,ngrid |
---|
| 420 | zkh(ig,ilev) = max(kmixmin,zkh(ig,ilev)) |
---|
| 421 | zkv(ig,ilev) = max(kmixmin,zkv(ig,ilev)) |
---|
| 422 | end do |
---|
| 423 | end do |
---|
| 424 | end if |
---|
| 425 | |
---|
| 426 | c ** diagnostique pour le schema de turbulence |
---|
| 427 | c ----------------------------------------- |
---|
| 428 | |
---|
| 429 | IF(lecrit) THEN |
---|
| 430 | PRINT* |
---|
| 431 | PRINT*,'Diagnostic for the vertical turbulent mixing' |
---|
| 432 | PRINT*,'Cd for momentum and potential temperature' |
---|
| 433 | |
---|
| 434 | PRINT*,zcdv(ngrid/2+1),zcdh(ngrid/2+1) |
---|
| 435 | PRINT*,'Mixing coefficient for momentum and pot.temp.' |
---|
| 436 | DO ilev=1,nlay |
---|
| 437 | PRINT*,zkv(ngrid/2+1,ilev),zkh(ngrid/2+1,ilev) |
---|
| 438 | ENDDO |
---|
| 439 | ENDIF |
---|
| 440 | |
---|
| 441 | |
---|
| 442 | |
---|
| 443 | |
---|
| 444 | c----------------------------------------------------------------------- |
---|
| 445 | c 4. inversion pour l'implicite sur u |
---|
| 446 | c -------------------------------- |
---|
| 447 | |
---|
| 448 | c ** l'equation est |
---|
| 449 | c u(t+1) = u(t) + dt * {(du/dt)phys}(t) + dt * {(du/dt)difv}(t+1) |
---|
| 450 | c avec |
---|
| 451 | c /zu/ = u(t) + dt * {(du/dt)phys}(t) (voir paragraphe 2.) |
---|
| 452 | c et |
---|
| 453 | c dt * {(du/dt)difv}(t+1) = dt * {(d/dz)[ Ku (du/dz) ]}(t+1) |
---|
| 454 | c donc les entrees sont /zcdv/ pour la condition a la limite sol |
---|
| 455 | c et /zkv/ = Ku |
---|
[2312] | 456 | |
---|
[2274] | 457 | zb(1:ngrid,2:nlay)=zkv(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
| 458 | zb(1:ngrid,1)=zcdv(1:ngrid)*zb0(1:ngrid,1) |
---|
[38] | 459 | |
---|
| 460 | DO ig=1,ngrid |
---|
| 461 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
| 462 | zc(ig,nlay)=za(ig,nlay)*zu(ig,nlay)*z1(ig) |
---|
| 463 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
| 464 | ENDDO |
---|
| 465 | |
---|
| 466 | DO ilay=nlay-1,1,-1 |
---|
| 467 | DO ig=1,ngrid |
---|
| 468 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
| 469 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
| 470 | zc(ig,ilay)=(za(ig,ilay)*zu(ig,ilay)+ |
---|
| 471 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
| 472 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
| 473 | ENDDO |
---|
| 474 | ENDDO |
---|
| 475 | |
---|
| 476 | DO ig=1,ngrid |
---|
| 477 | zu(ig,1)=zc(ig,1) |
---|
| 478 | ENDDO |
---|
| 479 | DO ilay=2,nlay |
---|
| 480 | DO ig=1,ngrid |
---|
| 481 | zu(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zu(ig,ilay-1) |
---|
| 482 | ENDDO |
---|
| 483 | ENDDO |
---|
| 484 | |
---|
| 485 | |
---|
| 486 | |
---|
| 487 | |
---|
| 488 | |
---|
| 489 | c----------------------------------------------------------------------- |
---|
| 490 | c 5. inversion pour l'implicite sur v |
---|
| 491 | c -------------------------------- |
---|
| 492 | |
---|
| 493 | c ** l'equation est |
---|
| 494 | c v(t+1) = v(t) + dt * {(dv/dt)phys}(t) + dt * {(dv/dt)difv}(t+1) |
---|
| 495 | c avec |
---|
| 496 | c /zv/ = v(t) + dt * {(dv/dt)phys}(t) (voir paragraphe 2.) |
---|
| 497 | c et |
---|
| 498 | c dt * {(dv/dt)difv}(t+1) = dt * {(d/dz)[ Kv (dv/dz) ]}(t+1) |
---|
| 499 | c donc les entrees sont /zcdv/ pour la condition a la limite sol |
---|
| 500 | c et /zkv/ = Kv |
---|
| 501 | |
---|
| 502 | DO ig=1,ngrid |
---|
| 503 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
| 504 | zc(ig,nlay)=za(ig,nlay)*zv(ig,nlay)*z1(ig) |
---|
| 505 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
| 506 | ENDDO |
---|
| 507 | |
---|
| 508 | DO ilay=nlay-1,1,-1 |
---|
| 509 | DO ig=1,ngrid |
---|
| 510 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
| 511 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
| 512 | zc(ig,ilay)=(za(ig,ilay)*zv(ig,ilay)+ |
---|
| 513 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
| 514 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
| 515 | ENDDO |
---|
| 516 | ENDDO |
---|
| 517 | |
---|
| 518 | DO ig=1,ngrid |
---|
| 519 | zv(ig,1)=zc(ig,1) |
---|
| 520 | ENDDO |
---|
| 521 | DO ilay=2,nlay |
---|
| 522 | DO ig=1,ngrid |
---|
| 523 | zv(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zv(ig,ilay-1) |
---|
| 524 | ENDDO |
---|
| 525 | ENDDO |
---|
| 526 | |
---|
| 527 | |
---|
| 528 | |
---|
| 529 | |
---|
| 530 | |
---|
| 531 | c----------------------------------------------------------------------- |
---|
| 532 | c 6. inversion pour l'implicite sur h sans oublier le couplage |
---|
| 533 | c avec le sol (conduction) |
---|
| 534 | c ------------------------ |
---|
| 535 | |
---|
| 536 | c ** l'equation est |
---|
| 537 | c h(t+1) = h(t) + dt * {(dh/dt)phys}(t) + dt * {(dh/dt)difv}(t+1) |
---|
| 538 | c avec |
---|
| 539 | c /zh/ = h(t) + dt * {(dh/dt)phys}(t) (voir paragraphe 2.) |
---|
| 540 | c et |
---|
| 541 | c dt * {(dh/dt)difv}(t+1) = dt * {(d/dz)[ Kh (dh/dz) ]}(t+1) |
---|
| 542 | c donc les entrees sont /zcdh/ pour la condition de raccord au sol |
---|
| 543 | c et /zkh/ = Kh |
---|
| 544 | c ------------- |
---|
| 545 | |
---|
[473] | 546 | c Mass variation scheme: |
---|
[2274] | 547 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
| 548 | zb(1:ngrid,1)=zcdh(1:ngrid)*zb0(1:ngrid,1) |
---|
[38] | 549 | |
---|
[473] | 550 | c on initialise dm c |
---|
| 551 | |
---|
| 552 | pdtc(:,:)=0. |
---|
| 553 | zt(:,:)=0. |
---|
| 554 | dmice(:,:)=0. |
---|
[38] | 555 | |
---|
| 556 | c ** calcul de (d Planck / dT) a la temperature d'interface |
---|
| 557 | c ------------------------------------------------------ |
---|
| 558 | |
---|
| 559 | z4st=4.*5.67e-8*ptimestep |
---|
[544] | 560 | IF (tke_heat_flux .eq. 0.) THEN |
---|
[38] | 561 | DO ig=1,ngrid |
---|
| 562 | zdplanck(ig)=z4st*pemis(ig)*ptsrf(ig)*ptsrf(ig)*ptsrf(ig) |
---|
| 563 | ENDDO |
---|
[544] | 564 | ELSE |
---|
| 565 | zdplanck(:)=0. |
---|
| 566 | ENDIF |
---|
[38] | 567 | |
---|
[473] | 568 | ! calcul de zc et zd pour la couche top en prenant en compte le terme |
---|
[2080] | 569 | ! de variation de masse (on fait une boucle pour que \E7a converge) |
---|
[473] | 570 | |
---|
| 571 | ! Identification des points de grilles qui ont besoin de la correction |
---|
| 572 | |
---|
| 573 | llnt(:)=1 |
---|
[1236] | 574 | IF (.not.turb_resolved) THEN |
---|
[884] | 575 | IF (callcond) THEN |
---|
| 576 | DO ig=1,ngrid |
---|
[473] | 577 | DO l=1,nlay |
---|
| 578 | if(zh(ig,l) .lt. zhcond(ig,l)) then |
---|
| 579 | llnt(ig)=300 |
---|
| 580 | ! 200 and 100 do not go beyond month 9 with normal dissipation |
---|
| 581 | goto 5 |
---|
| 582 | endif |
---|
| 583 | ENDDO |
---|
[884] | 584 | 5 continue |
---|
| 585 | ENDDO |
---|
| 586 | ENDIF |
---|
[473] | 587 | |
---|
[529] | 588 | ENDIF |
---|
| 589 | |
---|
[473] | 590 | DO ig=1,ngrid |
---|
| 591 | |
---|
| 592 | ! Initialization of z1 and zd, which do not depend on dmice |
---|
| 593 | |
---|
| 594 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
| 595 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
| 596 | |
---|
| 597 | DO ilay=nlay-1,1,-1 |
---|
| 598 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
| 599 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
| 600 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
| 601 | ENDDO |
---|
| 602 | |
---|
| 603 | ! Convergence loop |
---|
| 604 | |
---|
| 605 | DO j=1,llnt(ig) |
---|
| 606 | |
---|
| 607 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
| 608 | zc(ig,nlay)=za(ig,nlay)*zh(ig,nlay) |
---|
| 609 | & -betam(ig,nlay)*dmice(ig,nlay) |
---|
| 610 | zc(ig,nlay)=zc(ig,nlay)*z1(ig) |
---|
| 611 | ! zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
| 612 | |
---|
| 613 | ! calcul de zc et zd pour les couches du haut vers le bas |
---|
| 614 | |
---|
| 615 | DO ilay=nlay-1,1,-1 |
---|
| 616 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
| 617 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
| 618 | zc(ig,ilay)=(za(ig,ilay)*zh(ig,ilay)+ |
---|
| 619 | $ zb(ig,ilay+1)*zc(ig,ilay+1)- |
---|
| 620 | $ betam(ig,ilay)*dmice(ig,ilay))*z1(ig) |
---|
| 621 | ! zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
| 622 | ENDDO |
---|
| 623 | |
---|
[38] | 624 | c ** calcul de la temperature_d'interface et de sa tendance. |
---|
| 625 | c on ecrit que la somme des flux est nulle a l'interface |
---|
| 626 | c a t + \delta t, |
---|
| 627 | c c'est a dire le flux radiatif a {t + \delta t} |
---|
| 628 | c + le flux turbulent a {t + \delta t} |
---|
| 629 | c qui s'ecrit K (T1-Tsurf) avec T1 = d1 Tsurf + c1 |
---|
| 630 | c (notation K dt = /cpp*b/) |
---|
| 631 | c + le flux dans le sol a t |
---|
| 632 | c + l'evolution du flux dans le sol lorsque la temperature d'interface |
---|
| 633 | c passe de sa valeur a t a sa valeur a {t + \delta t}. |
---|
| 634 | c ---------------------------------------------------- |
---|
| 635 | |
---|
| 636 | z1(ig)=pcapcal(ig)*ptsrf(ig)+cpp*zb(ig,1)*zc(ig,1) |
---|
| 637 | s +zdplanck(ig)*ptsrf(ig)+ pfluxsrf(ig)*ptimestep |
---|
| 638 | z2(ig)= pcapcal(ig)+cpp*zb(ig,1)*(1.-zd(ig,1))+zdplanck(ig) |
---|
| 639 | ztsrf2(ig)=z1(ig)/z2(ig) |
---|
[473] | 640 | ! pdtsrf(ig)=(ztsrf2(ig)-ptsrf(ig))/ptimestep !incremented outside loop |
---|
| 641 | zhs(ig,1)=zc(ig,1)+zd(ig,1)*ztsrf2(ig) |
---|
[38] | 642 | |
---|
| 643 | c ** et a partir de la temperature au sol on remonte |
---|
| 644 | c ----------------------------------------------- |
---|
| 645 | |
---|
[473] | 646 | DO ilay=2,nlay |
---|
| 647 | zhs(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zhs(ig,ilay-1) |
---|
| 648 | ENDDO |
---|
| 649 | DO ilay=1,nlay |
---|
| 650 | zt(ig,ilay)=zhs(ig,ilay)*ppopsk(ig,ilay) |
---|
| 651 | ENDDO |
---|
| 652 | |
---|
| 653 | c Condensation/sublimation in the atmosphere |
---|
| 654 | c ------------------------------------------ |
---|
| 655 | c (computation of zcondicea and dmice) |
---|
| 656 | |
---|
[1996] | 657 | IF (.NOT. co2clouds) then |
---|
| 658 | DO l=nlay , 1, -1 |
---|
[473] | 659 | IF(zt(ig,l).LT.ztcond(ig,l)) THEN |
---|
| 660 | pdtc(ig,l)=(ztcond(ig,l) - zt(ig,l))/ptimestep |
---|
| 661 | zcondicea(ig,l)=(pplev(ig,l)-pplev(ig,l+1)) |
---|
| 662 | & *ccond*pdtc(ig,l) |
---|
| 663 | dmice(ig,l)= dmice(ig,l) + zcondicea(ig,l)*ptimestep |
---|
| 664 | END IF |
---|
[1996] | 665 | ENDDO |
---|
| 666 | ELSE |
---|
| 667 | DO l=nlay , 1, -1 |
---|
| 668 | zcondicea(ig,l)= 0.!pcondicea_co2microp(ig,l)* |
---|
| 669 | c & (pplev(ig,l) - pplev(ig,l+1))/g |
---|
| 670 | dmice(ig,l)= 0.!dmice(ig,l) + zcondicea(ig,l)*ptimestep |
---|
| 671 | pdtc(ig,l)=0. |
---|
| 672 | ENDDO |
---|
| 673 | ENDIF |
---|
| 674 | |
---|
| 675 | ENDDO!of Do j=1,XXX |
---|
[38] | 676 | |
---|
[1996] | 677 | ENDDO !of Do ig=1,ngrid |
---|
[38] | 678 | |
---|
[473] | 679 | pdtsrf(:)=(ztsrf2(:)-ptsrf(:))/ptimestep |
---|
[669] | 680 | |
---|
[660] | 681 | DO ig=1,ngrid ! computing sensible heat flux (atm => surface) |
---|
| 682 | sensibFlux(ig)=cpp*zb(ig,1)/ptimestep*(zhs(ig,1)-ztsrf2(ig)) |
---|
| 683 | ENDDO |
---|
[473] | 684 | |
---|
[38] | 685 | c----------------------------------------------------------------------- |
---|
| 686 | c TRACERS |
---|
| 687 | c ------- |
---|
| 688 | |
---|
| 689 | if(tracer) then |
---|
| 690 | |
---|
| 691 | c Using the wind modified by friction for lifting and sublimation |
---|
| 692 | c ---------------------------------------------------------------- |
---|
| 693 | |
---|
[529] | 694 | ! This is computed above and takes into account surface-atmosphere flux |
---|
| 695 | ! enhancement by subgrid gustiness and atmospheric-stability related |
---|
| 696 | ! variations of transfer coefficients. |
---|
| 697 | |
---|
| 698 | ! DO ig=1,ngrid |
---|
| 699 | ! zu2(ig)=zu(ig,1)*zu(ig,1)+zv(ig,1)*zv(ig,1) |
---|
| 700 | ! zcdv(ig)=zcdv_true(ig)*sqrt(zu2(ig)) |
---|
| 701 | ! zcdh(ig)=zcdh_true(ig)*sqrt(zu2(ig)) |
---|
| 702 | ! ENDDO |
---|
| 703 | |
---|
[38] | 704 | c Calcul du flux vertical au bas de la premiere couche (dust) : |
---|
| 705 | c ----------------------------------------------------------- |
---|
[1047] | 706 | do ig=1,ngrid |
---|
[38] | 707 | rho(ig) = zb0(ig,1) /ptimestep |
---|
| 708 | c zb(ig,1) = 0. |
---|
| 709 | end do |
---|
| 710 | c Dust lifting: |
---|
| 711 | if (lifting) then |
---|
[310] | 712 | #ifndef MESOSCALE |
---|
[38] | 713 | if (doubleq.AND.submicron) then |
---|
| 714 | do ig=1,ngrid |
---|
| 715 | c if(co2ice(ig).lt.1) then |
---|
| 716 | pdqsdif(ig,igcm_dust_mass) = |
---|
| 717 | & -alpha_lift(igcm_dust_mass) |
---|
| 718 | pdqsdif(ig,igcm_dust_number) = |
---|
| 719 | & -alpha_lift(igcm_dust_number) |
---|
| 720 | pdqsdif(ig,igcm_dust_submicron) = |
---|
| 721 | & -alpha_lift(igcm_dust_submicron) |
---|
| 722 | c end if |
---|
| 723 | end do |
---|
| 724 | else if (doubleq) then |
---|
[1974] | 725 | if (dustinjection.eq.0) then !injection scheme 0 (old) |
---|
| 726 | !or 2 (injection in CL) |
---|
| 727 | do ig=1,ngrid |
---|
[1455] | 728 | if(co2ice(ig).lt.1) then ! pas de soulevement si glace CO2 |
---|
[38] | 729 | pdqsdif(ig,igcm_dust_mass) = |
---|
| 730 | & -alpha_lift(igcm_dust_mass) |
---|
| 731 | pdqsdif(ig,igcm_dust_number) = |
---|
[520] | 732 | & -alpha_lift(igcm_dust_number) |
---|
| 733 | end if |
---|
[1974] | 734 | end do |
---|
| 735 | elseif(dustinjection.eq.1)then ! dust injection scheme = 1 injection from surface |
---|
| 736 | do ig=1,ngrid |
---|
| 737 | if(co2ice(ig).lt.1) then ! pas de soulevement si glace CO2 |
---|
[2160] | 738 | IF((ti_injection_sol.LE.local_time(ig)).and. |
---|
| 739 | & (local_time(ig).LE.tf_injection_sol)) THEN |
---|
[1974] | 740 | if (rdstorm) then !Rocket dust storm scheme |
---|
| 741 | pdqsdif(ig,igcm_stormdust_mass) = |
---|
| 742 | & -alpha_lift(igcm_stormdust_mass) |
---|
| 743 | & *dustliftday(ig) |
---|
| 744 | pdqsdif(ig,igcm_stormdust_number) = |
---|
| 745 | & -alpha_lift(igcm_stormdust_number) |
---|
| 746 | & *dustliftday(ig) |
---|
| 747 | pdqsdif(ig,igcm_dust_mass)= 0. |
---|
| 748 | pdqsdif(ig,igcm_dust_number)= 0. |
---|
| 749 | else |
---|
| 750 | pdqsdif(ig,igcm_dust_mass)= |
---|
| 751 | & -dustliftday(ig)* |
---|
| 752 | & alpha_lift(igcm_dust_mass) |
---|
| 753 | pdqsdif(ig,igcm_dust_number)= |
---|
| 754 | & -dustliftday(ig)* |
---|
| 755 | & alpha_lift(igcm_dust_number) |
---|
| 756 | endif |
---|
| 757 | if (submicron) then |
---|
| 758 | pdqsdif(ig,igcm_dust_submicron) = 0. |
---|
| 759 | endif ! if (submicron) |
---|
| 760 | ELSE ! outside dust injection time frame |
---|
[2080] | 761 | pdqsdif(ig,igcm_dust_mass)= 0. |
---|
| 762 | pdqsdif(ig,igcm_dust_number)= 0. |
---|
| 763 | if (rdstorm) then |
---|
[1974] | 764 | pdqsdif(ig,igcm_stormdust_mass)= 0. |
---|
| 765 | pdqsdif(ig,igcm_stormdust_number)= 0. |
---|
[2080] | 766 | end if |
---|
[1974] | 767 | ENDIF |
---|
| 768 | |
---|
| 769 | end if ! of if(co2ice(ig).lt.1) |
---|
| 770 | end do |
---|
| 771 | endif ! end if dustinjection |
---|
[38] | 772 | else if (submicron) then |
---|
| 773 | do ig=1,ngrid |
---|
| 774 | pdqsdif(ig,igcm_dust_submicron) = |
---|
| 775 | & -alpha_lift(igcm_dust_submicron) |
---|
| 776 | end do |
---|
| 777 | else |
---|
[1236] | 778 | #endif |
---|
[38] | 779 | call dustlift(ngrid,nlay,nq,rho,zcdh_true,zcdh,co2ice, |
---|
| 780 | & pdqsdif) |
---|
[1236] | 781 | #ifndef MESOSCALE |
---|
[38] | 782 | endif !doubleq.AND.submicron |
---|
[310] | 783 | #endif |
---|
[38] | 784 | else |
---|
| 785 | pdqsdif(1:ngrid,1:nq) = 0. |
---|
| 786 | end if |
---|
| 787 | |
---|
| 788 | c OU calcul de la valeur de q a la surface (water) : |
---|
| 789 | c ---------------------------------------- |
---|
| 790 | if (water) then |
---|
[1047] | 791 | call watersat(ngrid,ptsrf,pplev(1,1),qsat) |
---|
[38] | 792 | end if |
---|
| 793 | |
---|
| 794 | c Inversion pour l'implicite sur q |
---|
| 795 | c -------------------------------- |
---|
[1974] | 796 | do iq=1,nq !for all tracers including stormdust |
---|
[2274] | 797 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
[38] | 798 | |
---|
[2312] | 799 | if ((water).and.(iq.eq.igcm_h2o_vap)) then |
---|
[38] | 800 | c This line is required to account for turbulent transport |
---|
| 801 | c from surface (e.g. ice) to mid-layer of atmosphere: |
---|
[2274] | 802 | zb(1:ngrid,1)=zcdv(1:ngrid)*zb0(1:ngrid,1) |
---|
| 803 | zb(1:ngrid,1)=dryness(1:ngrid)*zb(1:ngrid,1) |
---|
[38] | 804 | else ! (re)-initialize zb(:,1) |
---|
| 805 | zb(1:ngrid,1)=0 |
---|
| 806 | end if |
---|
| 807 | |
---|
| 808 | DO ig=1,ngrid |
---|
| 809 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
| 810 | zc(ig,nlay)=za(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
| 811 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
| 812 | ENDDO |
---|
| 813 | |
---|
| 814 | DO ilay=nlay-1,2,-1 |
---|
| 815 | DO ig=1,ngrid |
---|
| 816 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
| 817 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
| 818 | zc(ig,ilay)=(za(ig,ilay)*zq(ig,ilay,iq)+ |
---|
| 819 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
| 820 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
| 821 | ENDDO |
---|
| 822 | ENDDO |
---|
| 823 | |
---|
[2312] | 824 | if ( (water.and.(iq.eq.igcm_h2o_ice)) |
---|
| 825 | $ .or. (hdo.and.(iq.eq.igcm_hdo_ice)) ) then |
---|
[38] | 826 | ! special case for water ice tracer: do not include |
---|
| 827 | ! h2o ice tracer from surface (which is set when handling |
---|
[473] | 828 | ! h2o vapour case (see further down). |
---|
[38] | 829 | DO ig=1,ngrid |
---|
| 830 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
| 831 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
| 832 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
| 833 | $ zb(ig,2)*zc(ig,2)) *z1(ig) |
---|
| 834 | ENDDO |
---|
[2312] | 835 | else if (hdo.and.(iq.eq.igcm_hdo_vap)) then |
---|
| 836 | CALL hdo_surfex(ngrid,nlay,nq,ptimestep, |
---|
| 837 | & zt,zq,pqsurf, |
---|
[2316] | 838 | & old_h2o_vap,pdqsdif,dwatercap_dif, |
---|
[2312] | 839 | & hdoflux) |
---|
| 840 | DO ig=1,ngrid |
---|
| 841 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
| 842 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
| 843 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
| 844 | $ zb(ig,2)*zc(ig,2) + |
---|
| 845 | $ (-hdoflux(ig)) *ptimestep) *z1(ig) !tracer flux from surface |
---|
| 846 | ENDDO |
---|
| 847 | |
---|
[38] | 848 | else ! general case |
---|
| 849 | DO ig=1,ngrid |
---|
| 850 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
| 851 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
| 852 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
| 853 | $ zb(ig,2)*zc(ig,2) + |
---|
| 854 | $ (-pdqsdif(ig,iq)) *ptimestep) *z1(ig) !tracer flux from surface |
---|
| 855 | ENDDO |
---|
[2312] | 856 | |
---|
[38] | 857 | endif ! of if (water.and.(iq.eq.igcm_h2o_ice)) |
---|
| 858 | |
---|
| 859 | IF ((water).and.(iq.eq.igcm_h2o_vap)) then |
---|
| 860 | c Calculation for turbulent exchange with the surface (for ice) |
---|
| 861 | DO ig=1,ngrid |
---|
[2312] | 862 | old_h2o_vap(ig)=zq(ig,1,igcm_h2o_vap) |
---|
[38] | 863 | zd(ig,1)=zb(ig,1)*z1(ig) |
---|
| 864 | zq1temp(ig)=zc(ig,1)+ zd(ig,1)*qsat(ig) |
---|
| 865 | |
---|
| 866 | pdqsdif(ig,igcm_h2o_ice)=rho(ig)*dryness(ig)*zcdv(ig) |
---|
| 867 | & *(zq1temp(ig)-qsat(ig)) |
---|
| 868 | c write(*,*)'flux vers le sol=',pdqsdif(ig,nq) |
---|
| 869 | END DO |
---|
| 870 | |
---|
| 871 | DO ig=1,ngrid |
---|
[2312] | 872 | IF (hdo) then !if hdo, need to treat polar caps differently |
---|
| 873 | h2oflux(ig) = pdqsdif(ig,igcm_h2o_ice) ! h2oflux is |
---|
| 874 | ! uncorrected waterflux |
---|
| 875 | ENDIF !hdo |
---|
| 876 | |
---|
[2260] | 877 | if ((-pdqsdif(ig,igcm_h2o_ice)*ptimestep) |
---|
| 878 | & .gt.(pqsurf(ig,igcm_h2o_ice))) then |
---|
| 879 | c write(*,*)'subliming more than available frost: qsurf!' |
---|
| 880 | if(watercaptag(ig)) then |
---|
| 881 | c dwatercap_dif same sign as pdqsdif (pos. toward ground) |
---|
[2316] | 882 | dwatercap_dif(ig) = pdqsdif(ig,igcm_h2o_ice) |
---|
| 883 | & + pqsurf(ig,igcm_h2o_ice)/ptimestep |
---|
[2260] | 884 | pdqsdif(ig,igcm_h2o_ice)= |
---|
[38] | 885 | & -pqsurf(ig,igcm_h2o_ice)/ptimestep |
---|
[2260] | 886 | c write(*,*) "subliming more than available frost: qsurf!" |
---|
| 887 | else ! (case not.watercaptag(ig)) |
---|
| 888 | pdqsdif(ig,igcm_h2o_ice)= |
---|
| 889 | & -pqsurf(ig,igcm_h2o_ice)/ptimestep |
---|
| 890 | dwatercap_dif(ig) = 0.0 |
---|
[2312] | 891 | if (hdo) then |
---|
| 892 | h2oflux(ig) = pdqsdif(ig,igcm_h2o_ice) |
---|
| 893 | endif |
---|
[2260] | 894 | |
---|
[38] | 895 | c write(*,*)'flux vers le sol=',pdqsdif(ig,nq) |
---|
| 896 | z1(ig)=1./(za(ig,1)+ zb(ig,2)*(1.-zd(ig,2))) |
---|
| 897 | zc(ig,1)=(za(ig,1)*zq(ig,1,igcm_h2o_vap)+ |
---|
[2316] | 898 | $ zb(ig,2)*zc(ig,2) + |
---|
| 899 | $ (-pdqsdif(ig,igcm_h2o_ice)) *ptimestep) *z1(ig) |
---|
[38] | 900 | zq1temp(ig)=zc(ig,1) |
---|
[2316] | 901 | endif !if .not.watercaptag(ig) |
---|
| 902 | endif ! if sublim more than surface |
---|
| 903 | |
---|
[38] | 904 | c Starting upward calculations for water : |
---|
[669] | 905 | zq(ig,1,igcm_h2o_vap)=zq1temp(ig) |
---|
| 906 | |
---|
[742] | 907 | !c Take into account H2O latent heat in surface energy budget |
---|
| 908 | !c We solve dT/dt = (2834.3-0.28*(T-To)-0.004*(T-To)^2)*1e3*iceflux/cpp |
---|
| 909 | ! tsrf_lw(ig) = ptsrf(ig) + pdtsrf(ig) *ptimestep |
---|
| 910 | ! |
---|
| 911 | ! alpha = exp(-4*abs(T1-T2)*pdqsdif(ig,igcm_h2o_ice) |
---|
| 912 | ! & *ptimestep/pcapcal(ig)) |
---|
| 913 | ! |
---|
| 914 | ! tsrf_lw(ig) = (tsrf_lw(ig)*(T2-alpha*T1)+T1*T2*(alpha-1)) |
---|
| 915 | ! & /(tsrf_lw(ig)*(1-alpha)+alpha*T2-T1) ! surface temperature at t+1 |
---|
| 916 | ! |
---|
| 917 | ! pdtsrf(ig) = (tsrf_lw(ig)-ptsrf(ig))/ptimestep |
---|
[2179] | 918 | c Take into account the H2O latent heat impact on the surface temperature |
---|
[2218] | 919 | if (latentheat_surfwater) then |
---|
[2179] | 920 | tsrf_lh(ig) = ptsrf(ig) + pdtsrf(ig) *ptimestep |
---|
| 921 | lh=(2834.3-0.28*(tsrf_lh(ig)-To)- |
---|
| 922 | & 0.004*(tsrf_lh(ig)-To)*(tsrf_lh(ig)-To))*1.e+3 |
---|
[2260] | 923 | pdtsrf(ig)= pdtsrf(ig) + (dwatercap_dif(ig)+ |
---|
| 924 | & pdqsdif(ig,igcm_h2o_ice))*lh /pcapcal(ig) |
---|
[2179] | 925 | endif |
---|
[669] | 926 | |
---|
| 927 | if(pqsurf(ig,igcm_h2o_ice) |
---|
[2316] | 928 | & +pdqsdif(ig,igcm_h2o_ice)*ptimestep |
---|
[669] | 929 | & .gt.frost_albedo_threshold) ! if there is still ice, T cannot exceed To |
---|
| 930 | & pdtsrf(ig) = min(pdtsrf(ig),(To-ptsrf(ig))/ptimestep) ! ice melt case |
---|
| 931 | |
---|
[38] | 932 | ENDDO ! of DO ig=1,ngrid |
---|
| 933 | ELSE |
---|
| 934 | c Starting upward calculations for simple mixing of tracer (dust) |
---|
| 935 | DO ig=1,ngrid |
---|
| 936 | zq(ig,1,iq)=zc(ig,1) |
---|
| 937 | ENDDO |
---|
| 938 | END IF ! of IF ((water).and.(iq.eq.igcm_h2o_vap)) |
---|
| 939 | |
---|
| 940 | DO ilay=2,nlay |
---|
| 941 | DO ig=1,ngrid |
---|
[626] | 942 | zq(ig,ilay,iq)=zc(ig,ilay)+zd(ig,ilay)*zq(ig,ilay-1,iq) |
---|
[38] | 943 | ENDDO |
---|
| 944 | ENDDO |
---|
| 945 | enddo ! of do iq=1,nq |
---|
| 946 | end if ! of if(tracer) |
---|
| 947 | |
---|
[2312] | 948 | C Diagnostic output for HDO |
---|
| 949 | if (hdo) then |
---|
| 950 | CALL WRITEDIAGFI(ngrid,'hdoflux', |
---|
| 951 | & 'hdoflux', |
---|
| 952 | & ' ',2,hdoflux) |
---|
| 953 | CALL WRITEDIAGFI(ngrid,'h2oflux', |
---|
| 954 | & 'h2oflux', |
---|
| 955 | & ' ',2,h2oflux) |
---|
| 956 | endif |
---|
| 957 | |
---|
[38] | 958 | c----------------------------------------------------------------------- |
---|
| 959 | c 8. calcul final des tendances de la diffusion verticale |
---|
| 960 | c ---------------------------------------------------- |
---|
| 961 | |
---|
| 962 | DO ilev = 1, nlay |
---|
| 963 | DO ig=1,ngrid |
---|
| 964 | pdudif(ig,ilev)=( zu(ig,ilev)- |
---|
| 965 | $ (pu(ig,ilev)+pdufi(ig,ilev)*ptimestep) )/ptimestep |
---|
| 966 | pdvdif(ig,ilev)=( zv(ig,ilev)- |
---|
| 967 | $ (pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep) )/ptimestep |
---|
[473] | 968 | hh = ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
---|
| 969 | $ + (latcond*dmice(ig,ilev)/cpp)/ppopsk(ig,ilev) |
---|
| 970 | pdhdif(ig,ilev)=( zhs(ig,ilev)- hh )/ptimestep |
---|
[38] | 971 | ENDDO |
---|
| 972 | ENDDO |
---|
| 973 | |
---|
| 974 | if (tracer) then |
---|
| 975 | DO iq = 1, nq |
---|
| 976 | DO ilev = 1, nlay |
---|
| 977 | DO ig=1,ngrid |
---|
| 978 | pdqdif(ig,ilev,iq)=(zq(ig,ilev,iq)- |
---|
| 979 | $ (pq(ig,ilev,iq) + pdqfi(ig,ilev,iq)*ptimestep))/ptimestep |
---|
| 980 | ENDDO |
---|
| 981 | ENDDO |
---|
| 982 | ENDDO |
---|
| 983 | end if |
---|
| 984 | |
---|
| 985 | c ** diagnostique final |
---|
| 986 | c ------------------ |
---|
| 987 | |
---|
| 988 | IF(lecrit) THEN |
---|
| 989 | PRINT*,'In vdif' |
---|
| 990 | PRINT*,'Ts (t) and Ts (t+st)' |
---|
| 991 | WRITE(*,'(a10,3a15)') |
---|
| 992 | s 'theta(t)','theta(t+dt)','u(t)','u(t+dt)' |
---|
| 993 | PRINT*,ptsrf(ngrid/2+1),ztsrf2(ngrid/2+1) |
---|
| 994 | DO ilev=1,nlay |
---|
| 995 | WRITE(*,'(4f15.7)') |
---|
[473] | 996 | s ph(ngrid/2+1,ilev),zhs(ngrid/2+1,ilev), |
---|
[38] | 997 | s pu(ngrid/2+1,ilev),zu(ngrid/2+1,ilev) |
---|
| 998 | |
---|
| 999 | ENDDO |
---|
| 1000 | ENDIF |
---|
| 1001 | |
---|
[1036] | 1002 | END SUBROUTINE vdifc |
---|
[1969] | 1003 | |
---|
[2312] | 1004 | c==================================== |
---|
| 1005 | |
---|
| 1006 | |
---|
[1969] | 1007 | END MODULE vdifc_mod |
---|