subroutine turbdiff(ngrid,nlay,nq,rnat, & ptimestep,pcapcal,lecrit, & pplay,pplev,pzlay,pzlev,pz0, & pu,pv,pt,ppopsk,pq,ptsrf,pemis,pqsurf, & pdtfi,pdqfi,pfluxsrf, & Pdudif,pdvdif,pdtdif,pdtsrf,sensibFlux,pq2, & pdqdif,pdqevap,pdqsdif,flux_u,flux_v,lastcall) use watercommon_h, only : RLVTT, T_h2O_ice_liq, RCPD, mx_eau_sol,Psat_water use radcommon_h, only : sigma, glat use surfdat_h, only: dryness use tracer_h, only: igcm_h2o_vap, igcm_h2o_ice use comcstfi_mod, only: rcp, g, r, cpp use callkeys_mod, only: water,tracer,nosurf implicit none !================================================================== ! ! Purpose ! ------- ! Turbulent diffusion (mixing) for pot. T, U, V and tracers ! ! Implicit scheme ! We start by adding to variables x the physical tendencies ! already computed. We resolve the equation: ! ! x(t+1) = x(t) + dt * (dx/dt)phys(t) + dt * (dx/dt)difv(t+1) ! ! Authors ! ------- ! F. Hourdin, F. Forget, R. Fournier (199X) ! R. Wordsworth, B. Charnay (2010) ! J. Leconte (2012): To f90 ! - Rewritten the diffusion scheme to conserve total enthalpy ! by accounting for dissipation of turbulent kinetic energy. ! - Accounting for lost mean flow kinetic energy should come soon. ! !================================================================== !----------------------------------------------------------------------- ! declarations ! ------------ ! arguments ! --------- INTEGER,INTENT(IN) :: ngrid INTEGER,INTENT(IN) :: nlay REAL,INTENT(IN) :: ptimestep REAL,INTENT(IN) :: pplay(ngrid,nlay),pplev(ngrid,nlay+1) REAL,INTENT(IN) :: pzlay(ngrid,nlay),pzlev(ngrid,nlay+1) REAL,INTENT(IN) :: pu(ngrid,nlay),pv(ngrid,nlay) REAL,INTENT(IN) :: pt(ngrid,nlay),ppopsk(ngrid,nlay) REAL,INTENT(IN) :: ptsrf(ngrid) ! surface temperature (K) REAL,INTENT(IN) :: pemis(ngrid) REAL,INTENT(IN) :: pdtfi(ngrid,nlay) REAL,INTENT(IN) :: pfluxsrf(ngrid) REAL,INTENT(OUT) :: pdudif(ngrid,nlay),pdvdif(ngrid,nlay) REAL,INTENT(OUT) :: pdtdif(ngrid,nlay) REAL,INTENT(OUT) :: pdtsrf(ngrid) ! tendency (K/s) on surface temperature REAL,INTENT(OUT) :: sensibFlux(ngrid) REAL,INTENT(IN) :: pcapcal(ngrid) REAL,INTENT(INOUT) :: pq2(ngrid,nlay+1) REAL,INTENT(OUT) :: flux_u(ngrid),flux_v(ngrid) REAL,INTENT(IN) :: rnat(ngrid) LOGICAL,INTENT(IN) :: lastcall ! not used ! Arguments added for condensation logical,intent(in) :: lecrit ! not used. REAL,INTENT(IN) :: pz0 ! Tracers ! -------- integer,intent(in) :: nq real,intent(in) :: pqsurf(ngrid,nq) real,intent(in) :: pq(ngrid,nlay,nq), pdqfi(ngrid,nlay,nq) real,intent(out) :: pdqdif(ngrid,nlay,nq) real,intent(out) :: pdqsdif(ngrid,nq) ! local ! ----- integer ilev,ig,ilay,nlev REAL z4st,zdplanck(ngrid) REAL zkv(ngrid,nlay+1),zkh(ngrid,nlay+1) REAL zcdv(ngrid),zcdh(ngrid) REAL zcdv_true(ngrid),zcdh_true(ngrid) REAL zu(ngrid,nlay),zv(ngrid,nlay) REAL zh(ngrid,nlay),zt(ngrid,nlay) REAL ztsrf(ngrid) REAL z1(ngrid),z2(ngrid) REAL zmass(ngrid,nlay) REAL zfluxv(ngrid,nlay),zfluxt(ngrid,nlay),zfluxq(ngrid,nlay) REAL zb0(ngrid,nlay) REAL zExner(ngrid,nlay),zovExner(ngrid,nlay) REAL zcv(ngrid,nlay),zdv(ngrid,nlay) !inversion coefficient for winds REAL zct(ngrid,nlay),zdt(ngrid,nlay) !inversion coefficient for temperature REAL zcq(ngrid,nlay),zdq(ngrid,nlay) !inversion coefficient for tracers REAL zcst1 REAL zu2!, a REAL zcq0(ngrid),zdq0(ngrid) REAL zx_alf1(ngrid),zx_alf2(ngrid) LOGICAL,SAVE :: firstcall=.true. !$OMP THREADPRIVATE(firstcall) ! Tracers ! ------- INTEGER iq REAL zq(ngrid,nlay,nq) REAL zqnoevap(ngrid,nlay) !special for water case to compute where evaporated water goes. REAL pdqevap(ngrid,nlay) !special for water case to compute where evaporated water goes. REAL zdmassevap(ngrid) REAL rho(ngrid) ! near-surface air density REAL qsat(ngrid),psat(ngrid) REAL kmixmin ! Variables added for implicit latent heat inclusion ! -------------------------------------------------- real dqsat(ngrid), qsat_temp1, qsat_temp2,psat_temp integer, save :: ivap, iliq, iliq_surf,iice_surf ! also make liq for clarity on surface... !$OMP THREADPRIVATE(ivap,iliq,iliq_surf,iice_surf) real, parameter :: karman=0.4 real cd0, roughratio real dqsdif_total(ngrid) real zq0(ngrid) ! Coherence test ! -------------- IF (firstcall) THEN if(water)then ivap=igcm_h2o_vap iliq=igcm_h2o_ice iliq_surf=igcm_h2o_vap iice_surf=igcm_h2o_ice ! simply to make the code legible ! to be generalised else ivap=0 iliq=0 iliq_surf=0 iice_surf=0 ! simply to make the code legible endif sensibFlux(:)=0. firstcall=.false. ENDIF !----------------------------------------------------------------------- ! 1. Initialisation ! ----------------- nlev=nlay+1 ! Calculate rho*dz, (P/Ps)**(R/cp) and dt*rho/dz=dt*rho**2 g/dp ! with rho=p/RT=p/ (R Theta) (p/ps)**kappa ! --------------------------------------------- DO ilay=1,nlay DO ig=1,ngrid zmass(ig,ilay)=(pplev(ig,ilay)-pplev(ig,ilay+1))/glat(ig) zExner(ig,ilay)=(pplev(ig,ilay)/pplev(ig,1))**rcp zovExner(ig,ilay)=1./ppopsk(ig,ilay) ENDDO ENDDO zcst1=4.*g*ptimestep/(R*R) DO ilev=2,nlev-1 DO ig=1,ngrid zb0(ig,ilev)=pplev(ig,ilev)/(pt(ig,ilev-1)+pt(ig,ilev)) zb0(ig,ilev)=zcst1*zb0(ig,ilev)*zb0(ig,ilev)/(pplay(ig,ilev-1)-pplay(ig,ilev)) ENDDO ENDDO DO ig=1,ngrid zb0(ig,1)=ptimestep*pplev(ig,1)/(R*ptsrf(ig)) ENDDO dqsdif_total(:)=0.0 !----------------------------------------------------------------------- ! 2. Add the physical tendencies computed so far ! ---------------------------------------------- DO ilev=1,nlay DO ig=1,ngrid zu(ig,ilev)=pu(ig,ilev) zv(ig,ilev)=pv(ig,ilev) zt(ig,ilev)=pt(ig,ilev)+pdtfi(ig,ilev)*ptimestep zh(ig,ilev)=pt(ig,ilev)*zovExner(ig,ilev) !for call vdif_kc, but could be moved and computed there ENDDO ENDDO if(tracer) then DO iq =1, nq DO ilev=1,nlay DO ig=1,ngrid zq(ig,ilev,iq)=pq(ig,ilev,iq) + pdqfi(ig,ilev,iq)*ptimestep ENDDO ENDDO ENDDO if (water) then DO ilev=1,nlay DO ig=1,ngrid zqnoevap(ig,ilev)=pq(ig,ilev,ivap) + pdqfi(ig,ilev,ivap)*ptimestep ENDDO ENDDO Endif end if !----------------------------------------------------------------------- ! 3. Turbulence scheme ! -------------------- ! ! Source of turbulent kinetic energy at the surface ! ------------------------------------------------- ! Formula is Cd_0 = (karman / log[1+z1/z0])^2 DO ig=1,ngrid roughratio = 1. + pzlay(ig,1)/pz0 cd0 = karman/log(roughratio) cd0 = cd0*cd0 zcdv_true(ig) = cd0 zcdh_true(ig) = cd0 if(nosurf)then zcdv_true(ig)=0.D+0 !JL12 disable atm/surface momentum flux zcdh_true(ig)=0.D+0 !JL12 disable sensible heat flux endif ENDDO DO ig=1,ngrid zu2=pu(ig,1)*pu(ig,1)+pv(ig,1)*pv(ig,1) zcdv(ig)=zcdv_true(ig)*sqrt(zu2) zcdh(ig)=zcdh_true(ig)*sqrt(zu2) ENDDO ! Turbulent diffusion coefficients in the boundary layer ! ------------------------------------------------------ call vdif_kc(ngrid,nlay,ptimestep,g,pzlev,pzlay,pu,pv,zh,zcdv_true,pq2,zkv,zkh) !JL12 why not call vdif_kc with updated winds and temperature ! Adding eddy mixing to mimic 3D general circulation in 1D ! R. Wordsworth & F. Forget (2010) if ((ngrid.eq.1)) then kmixmin = 1.0e-2 ! minimum eddy mix coeff in 1D do ilev=1,nlay do ig=1,ngrid zkh(ig,ilev) = max(kmixmin,zkh(ig,ilev)) zkv(ig,ilev) = max(kmixmin,zkv(ig,ilev)) end do end do end if !JL12 change zkv at the surface by zcdv to calculate the surface momentum flux properly DO ig=1,ngrid zkv(ig,1)=zcdv(ig) ENDDO !we treat only winds, energy and tracers coefficients will be computed with upadted winds !JL12 calculate the flux coefficients (tables multiplied elements by elements) zfluxv(1:ngrid,1:nlay)=zkv(1:ngrid,1:nlay)*zb0(1:ngrid,1:nlay) !----------------------------------------------------------------------- ! 4. Implicit inversion of u ! -------------------------- ! u(t+1) = u(t) + dt * {(du/dt)phys}(t) + dt * {(du/dt)difv}(t+1) ! avec ! /zu/ = u(t) + dt * {(du/dt)phys}(t) (voir paragraphe 2.) ! et ! dt * {(du/dt)difv}(t+1) = dt * {(d/dz)[ Ku (du/dz) ]}(t+1) ! donc les entrees sont /zcdv/ pour la condition a la limite sol ! et /zkv/ = Ku DO ig=1,ngrid z1(ig)=1./(zmass(ig,nlay)+zfluxv(ig,nlay)) zcv(ig,nlay)=zmass(ig,nlay)*zu(ig,nlay)*z1(ig) zdv(ig,nlay)=zfluxv(ig,nlay)*z1(ig) ENDDO DO ilay=nlay-1,1,-1 DO ig=1,ngrid z1(ig)=1./(zmass(ig,ilay)+zfluxv(ig,ilay) + zfluxv(ig,ilay+1)*(1.-zdv(ig,ilay+1))) zcv(ig,ilay)=(zmass(ig,ilay)*zu(ig,ilay)+zfluxv(ig,ilay+1)*zcv(ig,ilay+1))*z1(ig) zdv(ig,ilay)=zfluxv(ig,ilay)*z1(ig) ENDDO ENDDO DO ig=1,ngrid zu(ig,1)=zcv(ig,1) ENDDO DO ilay=2,nlay DO ig=1,ngrid zu(ig,ilay)=zcv(ig,ilay)+zdv(ig,ilay)*zu(ig,ilay-1) ENDDO ENDDO !----------------------------------------------------------------------- ! 5. Implicit inversion of v ! -------------------------- ! v(t+1) = v(t) + dt * {(dv/dt)phys}(t) + dt * {(dv/dt)difv}(t+1) ! avec ! /zv/ = v(t) + dt * {(dv/dt)phys}(t) (voir paragraphe 2.) ! et ! dt * {(dv/dt)difv}(t+1) = dt * {(d/dz)[ Kv (dv/dz) ]}(t+1) ! donc les entrees sont /zcdv/ pour la condition a la limite sol ! et /zkv/ = Kv DO ig=1,ngrid z1(ig)=1./(zmass(ig,nlay)+zfluxv(ig,nlay)) zcv(ig,nlay)=zmass(ig,nlay)*zv(ig,nlay)*z1(ig) zdv(ig,nlay)=zfluxv(ig,nlay)*z1(ig) ENDDO DO ilay=nlay-1,1,-1 DO ig=1,ngrid z1(ig)=1./(zmass(ig,ilay)+zfluxv(ig,ilay)+zfluxv(ig,ilay+1)*(1.-zdv(ig,ilay+1))) zcv(ig,ilay)=(zmass(ig,ilay)*zv(ig,ilay)+zfluxv(ig,ilay+1)*zcv(ig,ilay+1))*z1(ig) zdv(ig,ilay)=zfluxv(ig,ilay)*z1(ig) ENDDO ENDDO DO ig=1,ngrid zv(ig,1)=zcv(ig,1) ENDDO DO ilay=2,nlay DO ig=1,ngrid zv(ig,ilay)=zcv(ig,ilay)+zdv(ig,ilay)*zv(ig,ilay-1) ENDDO ENDDO ! Calcul of wind stress DO ig=1,ngrid flux_u(ig) = zfluxv(ig,1)/ptimestep*zu(ig,1) flux_v(ig) = zfluxv(ig,1)/ptimestep*zv(ig,1) ENDDO !---------------------------------------------------------------------------- ! 6. Implicit inversion of h, not forgetting the coupling with the ground ! h(t+1) = h(t) + dt * {(dh/dt)phys}(t) + dt * {(dh/dt)difv}(t+1) ! avec ! /zh/ = h(t) + dt * {(dh/dt)phys}(t) (voir paragraphe 2.) ! et ! dt * {(dh/dt)difv}(t+1) = dt * {(d/dz)[ Kh (dh/dz) ]}(t+1) ! donc les entrees sont /zcdh/ pour la condition de raccord au sol ! et /zkh/ = Kh ! Using the wind modified by friction for lifting and sublimation ! --------------------------------------------------------------- DO ig=1,ngrid zu2 = zu(ig,1)*zu(ig,1)+zv(ig,1)*zv(ig,1) zcdv(ig) = zcdv_true(ig)*sqrt(zu2) zcdh(ig) = zcdh_true(ig)*sqrt(zu2) zkh(ig,1)= zcdh(ig) ENDDO ! JL12 calculate the flux coefficients (tables multiplied elements by elements) ! --------------------------------------------------------------- zfluxq(1:ngrid,1:nlay)=zkh(1:ngrid,1:nlay)*zb0(1:ngrid,1:nlay) !JL12 we save zfluxq which doesn't need the Exner factor zfluxt(1:ngrid,1:nlay)=zfluxq(1:ngrid,1:nlay)*zExner(1:ngrid,1:nlay) DO ig=1,ngrid z1(ig)=1./(zmass(ig,nlay)+zfluxt(ig,nlay)*zovExner(ig,nlay)) zct(ig,nlay)=zmass(ig,nlay)*zt(ig,nlay)*z1(ig) zdt(ig,nlay)=zfluxt(ig,nlay)*zovExner(ig,nlay-1)*z1(ig) ENDDO DO ilay=nlay-1,2,-1 DO ig=1,ngrid z1(ig)=1./(zmass(ig,ilay)+zfluxt(ig,ilay)*zovExner(ig,ilay)+ & zfluxt(ig,ilay+1)*(zovExner(ig,ilay)-zdt(ig,ilay+1)*zovExner(ig,ilay+1))) zct(ig,ilay)=(zmass(ig,ilay)*zt(ig,ilay)+zfluxt(ig,ilay+1)*zct(ig,ilay+1)*zovExner(ig,ilay+1))*z1(ig) zdt(ig,ilay)=zfluxt(ig,ilay)*z1(ig)*zovExner(ig,ilay-1) ENDDO ENDDO !JL12 we treat last point afterward because zovExner(ig,ilay-1) does not exist there DO ig=1,ngrid z1(ig)=1./(zmass(ig,1)+zfluxt(ig,1)*zovExner(ig,1)+ & zfluxt(ig,2)*(zovExner(ig,1)-zdt(ig,2)*zovExner(ig,2))) zct(ig,1)=(zmass(ig,1)*zt(ig,1)+zfluxt(ig,2)*zct(ig,2)*zovExner(ig,2))*z1(ig) zdt(ig,1)=zfluxt(ig,1)*z1(ig) ENDDO ! Calculate (d Planck / dT) at the interface temperature ! ------------------------------------------------------ z4st=4.0*sigma*ptimestep DO ig=1,ngrid zdplanck(ig)=z4st*pemis(ig)*ptsrf(ig)*ptsrf(ig)*ptsrf(ig) ENDDO ! Calculate temperature tendency at the interface (dry case) ! ---------------------------------------------------------- ! Sum of fluxes at interface at time t + \delta t gives change in T: ! radiative fluxes ! turbulent convective (sensible) heat flux ! flux (if any) from subsurface if(.not.water) then DO ig=1,ngrid z1(ig)=pcapcal(ig)*ptsrf(ig)+cpp*zfluxt(ig,1)*zct(ig,1)*zovExner(ig,1) & + pfluxsrf(ig)*ptimestep + zdplanck(ig)*ptsrf(ig) z2(ig) = pcapcal(ig)+zdplanck(ig)+cpp*zfluxt(ig,1)*(1.-zovExner(ig,1)*zdt(ig,1)) ztsrf(ig) = z1(ig) / z2(ig) pdtsrf(ig) = (ztsrf(ig) - ptsrf(ig))/ptimestep zt(ig,1) = zct(ig,1) + zdt(ig,1)*ztsrf(ig) ENDDO ! JL12 note that the black body radiative flux emitted by the surface has been updated by the implicit scheme ! Recalculate temperature to top of atmosphere, starting from ground ! ------------------------------------------------------------------ DO ilay=2,nlay DO ig=1,ngrid zt(ig,ilay)=zct(ig,ilay)+zdt(ig,ilay)*zt(ig,ilay-1) ENDDO ENDDO endif ! not water !----------------------------------------------------------------------- ! TRACERS (no vapour) ! ------- if(tracer) then ! Calculate vertical flux from the bottom to the first layer (dust) ! ----------------------------------------------------------------- do ig=1,ngrid rho(ig) = zb0(ig,1) /ptimestep end do pdqsdif(:,:)=0. ! Implicit inversion of q ! ----------------------- do iq=1,nq if (iq.ne.ivap) then DO ig=1,ngrid z1(ig)=1./(zmass(ig,nlay)+zfluxq(ig,nlay)) zcq(ig,nlay)=zmass(ig,nlay)*zq(ig,nlay,iq)*z1(ig) zdq(ig,nlay)=zfluxq(ig,nlay)*z1(ig) ENDDO DO ilay=nlay-1,2,-1 DO ig=1,ngrid z1(ig)=1./(zmass(ig,ilay)+zfluxq(ig,ilay)+zfluxq(ig,ilay+1)*(1.-zdq(ig,ilay+1))) zcq(ig,ilay)=(zmass(ig,ilay)*zq(ig,ilay,iq)+zfluxq(ig,ilay+1)*zcq(ig,ilay+1))*z1(ig) zdq(ig,ilay)=zfluxq(ig,ilay)*z1(ig) ENDDO ENDDO if ((water).and.(iq.eq.iliq)) then ! special case for condensed water tracer: do not include ! h2o ice tracer from surface (which is set when handling ! h2o vapour case (see further down). ! zb(ig,1)=0 if iq ne ivap DO ig=1,ngrid z1(ig)=1./(zmass(ig,1)+zfluxq(ig,2)*(1.-zdq(ig,2))) zcq(ig,1)=(zmass(ig,1)*zq(ig,1,iq)+zfluxq(ig,2)*zcq(ig,2))*z1(ig) ENDDO else ! general case do ig=1,ngrid z1(ig)=1./(zmass(ig,1)+zfluxq(ig,2)*(1.-zdq(ig,2))) zcq(ig,1)=(zmass(ig,1)*zq(ig,1,iq)+zfluxq(ig,2)*zcq(ig,2)+(-pdqsdif(ig,iq))*ptimestep)*z1(ig) ! tracer flux from surface ! currently pdqsdif always zero here, ! so last line is superfluous enddo endif ! of if (water.and.(iq.eq.igcm_h2o_ice)) ! Starting upward calculations for simple tracer mixing (e.g., dust) do ig=1,ngrid zq(ig,1,iq)=zcq(ig,1) end do do ilay=2,nlay do ig=1,ngrid zq(ig,ilay,iq)=zcq(ig,ilay)+zdq(ig,ilay)*zq(ig,ilay-1,iq) end do end do endif ! if (iq.ne.ivap) ! Calculate temperature tendency including latent heat term ! and assuming an infinite source of water on the ground ! ------------------------------------------------------------------ if (water.and.(iq.eq.ivap)) then ! compute evaporation efficiency do ig=1,ngrid if(nint(rnat(ig)).eq.1)then dryness(ig)=pqsurf(ig,iliq_surf)+pqsurf(ig,iice_surf) dryness(ig)=MIN(1.,2*dryness(ig)/mx_eau_sol) dryness(ig)=MAX(0.,dryness(ig)) endif enddo do ig=1,ngrid ! Calculate the value of qsat at the surface (water) call Psat_water(ptsrf(ig),pplev(ig,1),psat(ig),qsat(ig)) call Psat_water(ptsrf(ig)-0.0001,pplev(ig,1),psat_temp,qsat_temp1) call Psat_water(ptsrf(ig)+0.0001,pplev(ig,1),psat_temp,qsat_temp2) dqsat(ig)=(qsat_temp2-qsat_temp1)/0.0002 ! calculate dQsat / dT by finite differences ! we cannot use the updated temperature value yet... enddo ! coefficients for q do ig=1,ngrid z1(ig)=1./(zmass(ig,nlay)+zfluxq(ig,nlay)) zcq(ig,nlay)=zmass(ig,nlay)*zq(ig,nlay,iq)*z1(ig) zdq(ig,nlay)=zfluxq(ig,nlay)*z1(ig) enddo do ilay=nlay-1,2,-1 do ig=1,ngrid z1(ig)=1./(zmass(ig,ilay)+zfluxq(ig,ilay)+zfluxq(ig,ilay+1)*(1.-zdq(ig,ilay+1))) zcq(ig,ilay)=(zmass(ig,ilay)*zq(ig,ilay,iq)+zfluxq(ig,ilay+1)*zcq(ig,ilay+1))*z1(ig) zdq(ig,ilay)=zfluxq(ig,ilay)*z1(ig) enddo enddo do ig=1,ngrid z1(ig)=1./(zmass(ig,1)+zfluxq(ig,1)*dryness(ig)+zfluxq(ig,2)*(1.-zdq(ig,2))) zcq(ig,1)=(zmass(ig,1)*zq(ig,1,iq)+zfluxq(ig,2)*zcq(ig,2))*z1(ig) zdq(ig,1)=dryness(ig)*zfluxq(ig,1)*z1(ig) enddo do ig=1,ngrid !calculation of surface temperature zdq0(ig) = dqsat(ig) zcq0(ig) = qsat(ig)-dqsat(ig)*ptsrf(ig) z1(ig) = pcapcal(ig)*ptsrf(ig) +cpp*zfluxt(ig,1)*zct(ig,1)*zovExner(ig,1) & + zdplanck(ig)*ptsrf(ig) + pfluxsrf(ig)*ptimestep & + zfluxq(ig,1)*dryness(ig)*RLVTT*((zdq(ig,1)-1.0)*zcq0(ig)+zcq(ig,1)) z2(ig) = pcapcal(ig) + cpp*zfluxt(ig,1)*(1.-zovExner(ig,1)*zdt(ig,1)) & + zdplanck(ig)+zfluxq(ig,1)*dryness(ig)*RLVTT*zdq0(ig)*(1.0-zdq(ig,1)) ztsrf(ig) = z1(ig) / z2(ig) ! calculation of qs and q1 zq0(ig) = zcq0(ig)+zdq0(ig)*ztsrf(ig) zq(ig,1,iq) = zcq(ig,1)+zdq(ig,1)*zq0(ig) ! calculation of evaporation dqsdif_total(ig)=zfluxq(ig,1)*dryness(ig)*(zq(ig,1,ivap)-zq0(ig)) ! -------------------------------------------------------- ! Now check if we've taken too much water from the surface ! This can only occur on the continent ! If we do, we recompute Tsurf, T1 and q1 accordingly if((-dqsdif_total(ig).gt.(pqsurf(ig,iice_surf)+pqsurf(ig,iliq_surf))).and.rnat(ig).eq.1)then !water flux * ptimestep dqsdif_total(ig)=-(pqsurf(ig,iice_surf)+pqsurf(ig,iliq_surf)) !recompute surface temperature z1(ig) = pcapcal(ig)*ptsrf(ig) +cpp*zfluxq(ig,1)*zct(ig,1)*zovExner(ig,1) & + zdplanck(ig)*ptsrf(ig) + pfluxsrf(ig)*ptimestep & + RLVTT*dqsdif_total(ig) z2(ig) = pcapcal(ig) + cpp*zfluxq(ig,1)*(1.-zovExner(ig,1)*zdt(ig,1)) & + zdplanck(ig) ztsrf(ig) = z1(ig) / z2(ig) !recompute q1 with new water flux from surface zq(ig,1,iq) = (zmass(ig,1)*(pq(ig,1,iq)+ptimestep*pdqfi(ig,1,iq)) & +zfluxq(ig,2)*zcq(ig,2)-dqsdif_total(ig)) & / (zmass(ig,1)+(1.-zdq(ig,2))*zfluxq(ig,2)) end if ! calculation surface T tendency and T(1) pdtsrf(ig) = (ztsrf(ig) - ptsrf(ig))/ptimestep zt(ig,1) = zct(ig,1) + zdt(ig,1)*ztsrf(ig) enddo ! recalculate temperature and q(vap) to top of atmosphere, starting from ground do ilay=2,nlay do ig=1,ngrid zq(ig,ilay,iq)=zcq(ig,ilay)+zdq(ig,ilay)*zq(ig,ilay-1,iq) zt(ig,ilay)=zct(ig,ilay)+zdt(ig,ilay)*zt(ig,ilay-1) end do end do do ig=1,ngrid ! -------------------------------------------------------------------------- ! On the ocean, if T > 0 C then the vapour tendency must replace the ice one ! The surface vapour tracer is actually liquid. To make things difficult. if (nint(rnat(ig)).eq.0) then ! unfrozen ocean pdqsdif(ig,iliq_surf)=dqsdif_total(ig)/ptimestep pdqsdif(ig,iice_surf)=0.0 elseif (nint(rnat(ig)).eq.1) then ! (continent) ! If water is evaporating / subliming, we take it from ice before liquid ! -- is this valid?? if(dqsdif_total(ig).lt.0)then if (-dqsdif_total(ig).gt.pqsurf(ig,iice_surf))then pdqsdif(ig,iice_surf) = -pqsurf(ig,iice_surf)/ptimestep ! removes all the ice! pdqsdif(ig,iliq_surf) = dqsdif_total(ig)/ptimestep- pdqsdif(ig,iice_surf) ! take the remainder from the liquid instead else pdqsdif(ig,iice_surf)=dqsdif_total(ig)/ptimestep pdqsdif(ig,iliq_surf)=0. end if else !dqsdif_total(ig).ge.0 !If water vapour is condensing, we must decide whether it forms ice or liquid. if(ztsrf(ig).gt.T_h2O_ice_liq)then pdqsdif(ig,iice_surf)=0.0 pdqsdif(ig,iliq_surf)=dqsdif_total(ig)/ptimestep else pdqsdif(ig,iice_surf)=dqsdif_total(ig)/ptimestep pdqsdif(ig,iliq_surf)=0.0 endif endif elseif (nint(rnat(ig)).eq.2) then ! (continental glaciers) pdqsdif(ig,iliq_surf)=0.0 pdqsdif(ig,iice_surf)=dqsdif_total(ig)/ptimestep endif !rnat end do ! of DO ig=1,ngrid endif ! if (water et iq=ivap) end do ! of do iq=1,nq if (water) then ! special case where we recompute water mixing without any evaporation. ! The difference with the first calculation then tells us where evaporated water has gone DO ig=1,ngrid z1(ig)=1./(zmass(ig,nlay)+zfluxq(ig,nlay)) zcq(ig,nlay)=zmass(ig,nlay)*zqnoevap(ig,nlay)*z1(ig) zdq(ig,nlay)=zfluxq(ig,nlay)*z1(ig) ENDDO DO ilay=nlay-1,2,-1 DO ig=1,ngrid z1(ig)=1./(zmass(ig,ilay)+zfluxq(ig,ilay)+zfluxq(ig,ilay+1)*(1.-zdq(ig,ilay+1))) zcq(ig,ilay)=(zmass(ig,ilay)*zqnoevap(ig,ilay)+zfluxq(ig,ilay+1)*zcq(ig,ilay+1))*z1(ig) zdq(ig,ilay)=zfluxq(ig,ilay)*z1(ig) ENDDO ENDDO do ig=1,ngrid z1(ig)=1./(zmass(ig,1)+zfluxq(ig,2)*(1.-zdq(ig,2))) zcq(ig,1)=(zmass(ig,1)*zqnoevap(ig,1)+zfluxq(ig,2)*zcq(ig,2))*z1(ig) enddo ! Starting upward calculations for simple tracer mixing (e.g., dust) do ig=1,ngrid zqnoevap(ig,1)=zcq(ig,1) end do do ilay=2,nlay do ig=1,ngrid zqnoevap(ig,ilay)=zcq(ig,ilay)+zdq(ig,ilay)*zqnoevap(ig,ilay-1) end do end do endif ! if water endif ! tracer !----------------------------------------------------------------------- ! 8. Final calculation of the vertical diffusion tendencies ! ----------------------------------------------------------------- do ilev = 1, nlay do ig=1,ngrid pdudif(ig,ilev)=(zu(ig,ilev)-(pu(ig,ilev)))/ptimestep pdvdif(ig,ilev)=(zv(ig,ilev)-(pv(ig,ilev)))/ptimestep pdtdif(ig,ilev)=( zt(ig,ilev)- pt(ig,ilev))/ptimestep-pdtfi(ig,ilev) enddo enddo DO ig=1,ngrid ! computing sensible heat flux (atm => surface) sensibFlux(ig)=cpp*zfluxt(ig,1)/ptimestep*(zt(ig,1)*zovExner(ig,1)-ztsrf(ig)) ENDDO if (tracer) then do iq = 1, nq do ilev = 1, nlay do ig=1,ngrid pdqdif(ig,ilev,iq)=(zq(ig,ilev,iq)-(pq(ig,ilev,iq)+pdqfi(ig,ilev,iq)*ptimestep))/ptimestep enddo enddo enddo if (water) then do ilev = 1, nlay do ig=1,ngrid pdqevap(ig,ilev)=(zq(ig,ilev,ivap)-zqnoevap(ig,ilev))/ptimestep enddo enddo do ig=1,ngrid zdmassevap(ig)=SUM(pdqevap(ig,:)*zmass(ig,:))*ptimestep end do endif endif if(water)then call writediagfi(ngrid,'beta','Dryness coefficient',' ',2,dryness) if (tracer) then call writediagfi(ngrid,'dqevap','evaporated water vapor specific concentration','s-1',3,pdqevap) endif endif ! if(lastcall)then ! if(ngrid.eq.1)then ! print*,'Saving k.out...' ! OPEN(12,file='k.out',form='formatted') ! DO ilay=1,nlay ! write(12,*) zkh(1,ilay), pplay(1,ilay) ! ENDDO ! CLOSE(12) ! endif ! endif end