SUBROUTINE thermcell_2002(ngrid, nlay, ptimestep, iflag_thermals, pplay, & pplev, pphi, pu, pv, pt, po, pduadj, pdvadj, pdtadj, pdoadj, fm0, entr0, & fraca, wa_moy, r_aspect, l_mix, w2di, tho) USE dimphy USE write_field_phy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! Réécriture à partir d'un listing papier à Habas, le 14/02/00 ! le thermique est supposé homogène et dissipé par mélange avec ! son environnement. la longueur l_mix contrôle l'efficacité du ! mélange ! Le calcul du transport des différentes espèces se fait en prenant ! en compte: ! 1. un flux de masse montant ! 2. un flux de masse descendant ! 3. un entrainement ! 4. un detrainement ! ======================================================================= ! ----------------------------------------------------------------------- ! declarations: ! ------------- include "dimensions.h" include "YOMCST.h" ! arguments: ! ---------- INTEGER ngrid, nlay, w2di, iflag_thermals REAL tho REAL ptimestep, l_mix, r_aspect REAL pt(ngrid, nlay), pdtadj(ngrid, nlay) REAL pu(ngrid, nlay), pduadj(ngrid, nlay) REAL pv(ngrid, nlay), pdvadj(ngrid, nlay) REAL po(ngrid, nlay), pdoadj(ngrid, nlay) REAL pplay(ngrid, nlay), pplev(ngrid, nlay+1) REAL pphi(ngrid, nlay) REAL fraca(ngrid, nlay+1), zw2(ngrid, nlay+1) INTEGER, SAVE :: idetr = 3, lev_out = 1 !$OMP THREADPRIVATE(idetr,lev_out) ! local: ! ------ INTEGER, SAVE :: dvdq = 0, flagdq = 0, dqimpl = 1 LOGICAL, SAVE :: debut = .TRUE. !$OMP THREADPRIVATE(dvdq,flagdq,debut,dqimpl) INTEGER ig, k, l, lmax(klon, klev+1), lmaxa(klon), lmix(klon) REAL zmax(klon), zw, zz, ztva(klon, klev), zzz REAL zlev(klon, klev+1), zlay(klon, klev) REAL zh(klon, klev), zdhadj(klon, klev) REAL ztv(klon, klev) REAL zu(klon, klev), zv(klon, klev), zo(klon, klev) REAL wh(klon, klev+1) REAL wu(klon, klev+1), wv(klon, klev+1), wo(klon, klev+1) REAL zla(klon, klev+1) REAL zwa(klon, klev+1) REAL zld(klon, klev+1) REAL zwd(klon, klev+1) REAL zsortie(klon, klev) REAL zva(klon, klev) REAL zua(klon, klev) REAL zoa(klon, klev) REAL zha(klon, klev) REAL wa_moy(klon, klev+1) REAL fracc(klon, klev+1) REAL zf, zf2 REAL thetath2(klon, klev), wth2(klon, klev) ! common/comtherm/thetath2,wth2 REAL count_time LOGICAL sorties REAL rho(klon, klev), rhobarz(klon, klev+1), masse(klon, klev) REAL zpspsk(klon, klev) REAL wmax(klon, klev), wmaxa(klon) REAL wa(klon, klev, klev+1) REAL wd(klon, klev+1) REAL larg_part(klon, klev, klev+1) REAL fracd(klon, klev+1) REAL xxx(klon, klev+1) REAL larg_cons(klon, klev+1) REAL larg_detr(klon, klev+1) REAL fm0(klon, klev+1), entr0(klon, klev), detr(klon, klev) REAL pu_therm(klon, klev), pv_therm(klon, klev) REAL fm(klon, klev+1), entr(klon, klev) REAL fmc(klon, klev+1) CHARACTER (LEN=2) :: str2 CHARACTER (LEN=10) :: str10 CHARACTER (LEN=20) :: modname = 'thermcell2002' CHARACTER (LEN=80) :: abort_message LOGICAL vtest(klon), down EXTERNAL scopy INTEGER ncorrec, ll SAVE ncorrec DATA ncorrec/0/ !$OMP THREADPRIVATE(ncorrec) ! ----------------------------------------------------------------------- ! initialisation: ! --------------- sorties = .TRUE. IF (ngrid/=klon) THEN PRINT * PRINT *, 'STOP dans convadj' PRINT *, 'ngrid =', ngrid PRINT *, 'klon =', klon END IF ! ----------------------------------------------------------------------- ! incrementation eventuelle de tendances precedentes: ! --------------------------------------------------- ! print*,'0 OK convect8' DO l = 1, nlay DO ig = 1, ngrid zpspsk(ig, l) = (pplay(ig,l)/pplev(ig,1))**rkappa zh(ig, l) = pt(ig, l)/zpspsk(ig, l) zu(ig, l) = pu(ig, l) zv(ig, l) = pv(ig, l) zo(ig, l) = po(ig, l) ztv(ig, l) = zh(ig, l)*(1.+0.61*zo(ig,l)) END DO END DO ! print*,'1 OK convect8' ! -------------------- ! + + + + + + + + + + + ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz ! wh,wt,wo ... ! + + + + + + + + + + + zh,zu,zv,zo,rho ! -------------------- zlev(1) ! \\\\\\\\\\\\\\\\\\\\ ! ----------------------------------------------------------------------- ! Calcul des altitudes des couches ! ----------------------------------------------------------------------- IF (debut) THEN flagdq = (iflag_thermals-1000)/100 dvdq = (iflag_thermals-(1000+flagdq*100))/10 IF (flagdq==2) dqimpl = -1 IF (flagdq==3) dqimpl = 1 debut = .FALSE. END IF PRINT *, 'TH flag th ', iflag_thermals, flagdq, dvdq, dqimpl DO l = 2, nlay DO ig = 1, ngrid zlev(ig, l) = 0.5*(pphi(ig,l)+pphi(ig,l-1))/rg END DO END DO DO ig = 1, ngrid zlev(ig, 1) = 0. zlev(ig, nlay+1) = (2.*pphi(ig,klev)-pphi(ig,klev-1))/rg END DO DO l = 1, nlay DO ig = 1, ngrid zlay(ig, l) = pphi(ig, l)/rg END DO END DO ! print*,'2 OK convect8' ! ----------------------------------------------------------------------- ! Calcul des densites ! ----------------------------------------------------------------------- DO l = 1, nlay DO ig = 1, ngrid rho(ig, l) = pplay(ig, l)/(zpspsk(ig,l)*rd*zh(ig,l)) END DO END DO DO l = 2, nlay DO ig = 1, ngrid rhobarz(ig, l) = 0.5*(rho(ig,l)+rho(ig,l-1)) END DO END DO DO k = 1, nlay DO l = 1, nlay + 1 DO ig = 1, ngrid wa(ig, k, l) = 0. END DO END DO END DO ! print*,'3 OK convect8' ! ------------------------------------------------------------------ ! Calcul de w2, quarre de w a partir de la cape ! a partir de w2, on calcule wa, vitesse de l'ascendance ! ATTENTION: Dans cette version, pour cause d'economie de memoire, ! w2 est stoke dans wa ! ATTENTION: dans convect8, on n'utilise le calcule des wa ! independants par couches que pour calculer l'entrainement ! a la base et la hauteur max de l'ascendance. ! Indicages: ! l'ascendance provenant du niveau k traverse l'interface l avec ! une vitesse wa(k,l). ! -------------------- ! + + + + + + + + + + ! wa(k,l) ---- -------------------- l ! /\ ! /||\ + + + + + + + + + + ! || ! || -------------------- ! || ! || + + + + + + + + + + ! || ! || -------------------- ! ||__ ! |___ + + + + + + + + + + k ! -------------------- ! ------------------------------------------------------------------ DO k = 1, nlay - 1 DO ig = 1, ngrid wa(ig, k, k) = 0. wa(ig, k, k+1) = 2.*rg*(ztv(ig,k)-ztv(ig,k+1))/ztv(ig, k+1)* & (zlev(ig,k+1)-zlev(ig,k)) END DO DO l = k + 1, nlay - 1 DO ig = 1, ngrid wa(ig, k, l+1) = wa(ig, k, l) + 2.*rg*(ztv(ig,k)-ztv(ig,l))/ztv(ig, l & )*(zlev(ig,l+1)-zlev(ig,l)) END DO END DO DO ig = 1, ngrid wa(ig, k, nlay+1) = 0. END DO END DO ! print*,'4 OK convect8' ! Calcul de la couche correspondant a la hauteur du thermique DO k = 1, nlay - 1 DO ig = 1, ngrid lmax(ig, k) = k END DO DO l = nlay, k + 1, -1 DO ig = 1, ngrid IF (wa(ig,k,l)<=1.E-10) lmax(ig, k) = l - 1 END DO END DO END DO ! print*,'5 OK convect8' ! Calcule du w max du thermique DO k = 1, nlay DO ig = 1, ngrid wmax(ig, k) = 0. END DO END DO DO k = 1, nlay - 1 DO l = k, nlay DO ig = 1, ngrid IF (l<=lmax(ig,k)) THEN wa(ig, k, l) = sqrt(wa(ig,k,l)) wmax(ig, k) = max(wmax(ig,k), wa(ig,k,l)) ELSE wa(ig, k, l) = 0. END IF END DO END DO END DO DO k = 1, nlay - 1 DO ig = 1, ngrid pu_therm(ig, k) = sqrt(wmax(ig,k)) pv_therm(ig, k) = sqrt(wmax(ig,k)) END DO END DO ! print*,'6 OK convect8' ! Longueur caracteristique correspondant a la hauteur des thermiques. DO ig = 1, ngrid zmax(ig) = 500. END DO ! print*,'LMAX LMAX LMAX ' DO k = 1, nlay - 1 DO ig = 1, ngrid zmax(ig) = max(zmax(ig), zlev(ig,lmax(ig,k))-zlev(ig,k)) END DO ! print*,k,lmax(1,k) END DO ! print*,'ZMAX ZMAX ZMAX ',zmax ! call dump2d(iim,jjm-1,zmax(2:ngrid-1),'ZMAX ') ! print*,'OKl336' ! Calcul de l'entrainement. ! Le rapport d'aspect relie la largeur de l'ascendance a l'epaisseur ! de la couche d'alimentation en partant du principe que la vitesse ! maximum dans l'ascendance est la vitesse d'entrainement horizontale. DO k = 1, nlay DO ig = 1, ngrid zzz = rho(ig, k)*wmax(ig, k)*(zlev(ig,k+1)-zlev(ig,k))/ & (zmax(ig)*r_aspect) IF (w2di==2) THEN entr(ig, k) = entr(ig, k) + ptimestep*(zzz-entr(ig,k))/tho ELSE entr(ig, k) = zzz END IF ztva(ig, k) = ztv(ig, k) END DO END DO ! print*,'7 OK convect8' DO k = 1, klev + 1 DO ig = 1, ngrid zw2(ig, k) = 0. fmc(ig, k) = 0. larg_cons(ig, k) = 0. larg_detr(ig, k) = 0. wa_moy(ig, k) = 0. END DO END DO ! print*,'8 OK convect8' DO ig = 1, ngrid lmaxa(ig) = 1 lmix(ig) = 1 wmaxa(ig) = 0. END DO ! print*,'OKl372' DO l = 1, nlay - 2 DO ig = 1, ngrid ! if (zw2(ig,l).lt.1.e-10.and.ztv(ig,l).gt.ztv(ig,l+1)) then ! print*,'COUCOU ',l,zw2(ig,l),ztv(ig,l),ztv(ig,l+1) IF (zw2(ig,l)<1.E-10 .AND. ztv(ig,l)>ztv(ig,l+1) .AND. & entr(ig,l)>1.E-10) THEN ! print*,'COUCOU cas 1' ! Initialisation de l'ascendance ! lmix(ig)=1 ztva(ig, l) = ztv(ig, l) fmc(ig, l) = 0. fmc(ig, l+1) = entr(ig, l) zw2(ig, l) = 0. ! if (.not.ztv(ig,l+1).gt.150.) then ! print*,'ig,l+1,ztv(ig,l+1)' ! print*, ig,l+1,ztv(ig,l+1) ! endif zw2(ig, l+1) = 2.*rg*(ztv(ig,l)-ztv(ig,l+1))/ztv(ig, l+1)* & (zlev(ig,l+1)-zlev(ig,l)) larg_detr(ig, l) = 0. ELSE IF (zw2(ig,l)>=1.E-10 .AND. fmc(ig,l)+entr(ig,l)>1.E-10) THEN ! Incrementation... fmc(ig, l+1) = fmc(ig, l) + entr(ig, l) ! if (.not.fmc(ig,l+1).gt.1.e-15) then ! print*,'ig,l+1,fmc(ig,l+1)' ! print*, ig,l+1,fmc(ig,l+1) ! print*,'Fmc ',(fmc(ig,ll),ll=1,klev+1) ! print*,'W2 ',(zw2(ig,ll),ll=1,klev+1) ! print*,'Tv ',(ztv(ig,ll),ll=1,klev) ! print*,'Entr ',(entr(ig,ll),ll=1,klev) ! endif ztva(ig, l) = (fmc(ig,l)*ztva(ig,l-1)+entr(ig,l)*ztv(ig,l))/ & fmc(ig, l+1) ! mise a jour de la vitesse ascendante (l'air entraine de la couche ! consideree commence avec une vitesse nulle). zw2(ig, l+1) = zw2(ig, l)*(fmc(ig,l)/fmc(ig,l+1))**2 + & 2.*rg*(ztva(ig,l)-ztv(ig,l))/ztv(ig, l)*(zlev(ig,l+1)-zlev(ig,l)) END IF IF (zw2(ig,l+1)<0.) THEN zw2(ig, l+1) = 0. lmaxa(ig) = l ELSE wa_moy(ig, l+1) = sqrt(zw2(ig,l+1)) END IF IF (wa_moy(ig,l+1)>wmaxa(ig)) THEN ! lmix est le niveau de la couche ou w (wa_moy) est maximum lmix(ig) = l + 1 wmaxa(ig) = wa_moy(ig, l+1) END IF ! print*,'COUCOU cas 2 LMIX=',lmix(ig),wa_moy(ig,l+1),wmaxa(ig) END DO END DO ! print*,'9 OK convect8' ! print*,'WA1 ',wa_moy ! determination de l'indice du debut de la mixed layer ou w decroit ! calcul de la largeur de chaque ascendance dans le cas conservatif. ! dans ce cas simple, on suppose que la largeur de l'ascendance provenant ! d'une couche est égale à la hauteur de la couche alimentante. ! La vitesse maximale dans l'ascendance est aussi prise comme estimation ! de la vitesse d'entrainement horizontal dans la couche alimentante. ! print*,'OKl439' DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmaxa(ig)) THEN zw = max(wa_moy(ig,l), 1.E-10) larg_cons(ig, l) = zmax(ig)*r_aspect*fmc(ig, l)/(rhobarz(ig,l)*zw) END IF END DO END DO DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmaxa(ig)) THEN ! if (idetr.eq.0) then ! cette option est finalement en dur. larg_detr(ig, l) = sqrt(l_mix*zlev(ig,l)) ! else if (idetr.eq.1) then ! larg_detr(ig,l)=larg_cons(ig,l) ! s *sqrt(l_mix*zlev(ig,l))/larg_cons(ig,lmix(ig)) ! else if (idetr.eq.2) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *sqrt(wa_moy(ig,l)) ! else if (idetr.eq.4) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *wa_moy(ig,l) ! endif END IF END DO END DO ! print*,'10 OK convect8' ! print*,'WA2 ',wa_moy ! calcul de la fraction de la maille concernée par l'ascendance en tenant ! compte de l'epluchage du thermique. DO l = 2, nlay DO ig = 1, ngrid IF (larg_cons(ig,l)>1.) THEN ! print*,ig,l,lmix(ig),lmaxa(ig),larg_cons(ig,l),' KKK' fraca(ig, l) = (larg_cons(ig,l)-larg_detr(ig,l))/(r_aspect*zmax(ig)) IF (l>lmix(ig)) THEN xxx(ig, l) = (lmaxa(ig)+1.-l)/(lmaxa(ig)+1.-lmix(ig)) IF (idetr==0) THEN fraca(ig, l) = fraca(ig, lmix(ig)) ELSE IF (idetr==1) THEN fraca(ig, l) = fraca(ig, lmix(ig))*xxx(ig, l) ELSE IF (idetr==2) THEN fraca(ig, l) = fraca(ig, lmix(ig))*(1.-(1.-xxx(ig,l))**2) ELSE fraca(ig, l) = fraca(ig, lmix(ig))*xxx(ig, l)**2 END IF END IF ! print*,ig,l,lmix(ig),lmaxa(ig),xxx(ig,l),'LLLLLLL' fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) ELSE ! wa_moy(ig,l)=0. fraca(ig, l) = 0. fracc(ig, l) = 0. fracd(ig, l) = 1. END IF END DO END DO ! print*,'11 OK convect8' ! print*,'Ea3 ',wa_moy ! ------------------------------------------------------------------ ! Calcul de fracd, wd ! somme wa - wd = 0 ! ------------------------------------------------------------------ DO ig = 1, ngrid fm(ig, 1) = 0. fm(ig, nlay+1) = 0. END DO DO l = 2, nlay DO ig = 1, ngrid fm(ig, l) = fraca(ig, l)*wa_moy(ig, l)*rhobarz(ig, l) END DO DO ig = 1, ngrid IF (fracd(ig,l)<0.1) THEN abort_message = 'fracd trop petit' CALL abort_physic(modname, abort_message, 1) ELSE ! vitesse descendante "diagnostique" wd(ig, l) = fm(ig, l)/(fracd(ig,l)*rhobarz(ig,l)) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid ! masse(ig,l)=rho(ig,l)*(zlev(ig,l+1)-zlev(ig,l)) masse(ig, l) = (pplev(ig,l)-pplev(ig,l+1))/rg END DO END DO ! print*,'12 OK convect8' ! print*,'WA4 ',wa_moy ! c------------------------------------------------------------------ ! calcul du transport vertical ! ------------------------------------------------------------------ GO TO 4444 ! print*,'XXXXXXXXXXXXXXX ptimestep= ',ptimestep DO l = 2, nlay - 1 DO ig = 1, ngrid IF (fm(ig,l+1)*ptimestep>masse(ig,l) .AND. fm(ig,l+1)*ptimestep>masse( & ig,l+1)) THEN ! print*,'WARN!!! FM>M ig=',ig,' l=',l,' FM=' ! s ,fm(ig,l+1)*ptimestep ! s ,' M=',masse(ig,l),masse(ig,l+1) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (entr(ig,l)*ptimestep>masse(ig,l)) THEN ! print*,'WARN!!! E>M ig=',ig,' l=',l,' E==' ! s ,entr(ig,l)*ptimestep ! s ,' M=',masse(ig,l) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (.NOT. fm(ig,l)>=0. .OR. .NOT. fm(ig,l)<=10.) THEN ! print*,'WARN!!! fm exagere ig=',ig,' l=',l ! s ,' FM=',fm(ig,l) END IF IF (.NOT. masse(ig,l)>=1.E-10 .OR. .NOT. masse(ig,l)<=1.E4) THEN ! print*,'WARN!!! masse exagere ig=',ig,' l=',l ! s ,' M=',masse(ig,l) ! print*,'rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l)', ! s rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l) ! print*,'zlev(ig,l+1),zlev(ig,l)' ! s ,zlev(ig,l+1),zlev(ig,l) ! print*,'pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1)' ! s ,pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1) END IF IF (.NOT. entr(ig,l)>=0. .OR. .NOT. entr(ig,l)<=10.) THEN ! print*,'WARN!!! entr exagere ig=',ig,' l=',l ! s ,' E=',entr(ig,l) END IF END DO END DO 4444 CONTINUE ! print*,'OK 444 ' IF (w2di==1) THEN fm0 = fm0 + ptimestep*(fm-fm0)/tho entr0 = entr0 + ptimestep*(entr-entr0)/tho ELSE fm0 = fm entr0 = entr END IF IF (flagdq==0) THEN CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zh, zdhadj, & zha) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zo, pdoadj, & zoa) PRINT *, 'THERMALS OPT 1' ELSE IF (flagdq==1) THEN CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zh, & zdhadj, zha) CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zo, & pdoadj, zoa) PRINT *, 'THERMALS OPT 2' ELSE CALL thermcell_dq(ngrid, nlay, dqimpl, ptimestep, fm0, entr0, masse, zh, & zdhadj, zha, lev_out) CALL thermcell_dq(ngrid, nlay, dqimpl, ptimestep, fm0, entr0, masse, zo, & pdoadj, zoa, lev_out) PRINT *, 'THERMALS OPT 3', dqimpl END IF PRINT *, 'TH VENT ', dvdq IF (dvdq==0) THEN ! print*,'TH VENT OK ',dvdq CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zu, pduadj, & zua) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zv, pdvadj, & zva) ELSE IF (dvdq==1) THEN CALL dvthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zmax, & zu, zv, pduadj, pdvadj, zua, zva) ELSE IF (dvdq==2) THEN CALL thermcell_dv2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, & zmax, zu, zv, pduadj, pdvadj, zua, zva, lev_out) ELSE IF (dvdq==3) THEN CALL thermcell_dq(ngrid, nlay, dqimpl, ptimestep, fm0, entr0, masse, zu, & pduadj, zua, lev_out) CALL thermcell_dq(ngrid, nlay, dqimpl, ptimestep, fm0, entr0, masse, zv, & pdvadj, zva, lev_out) END IF ! CALL writefield_phy('duadj',pduadj,klev) DO l = 1, nlay DO ig = 1, ngrid zf = 0.5*(fracc(ig,l)+fracc(ig,l+1)) zf2 = zf/(1.-zf) thetath2(ig, l) = zf2*(zha(ig,l)-zh(ig,l))**2 wth2(ig, l) = zf2*(0.5*(wa_moy(ig,l)+wa_moy(ig,l+1)))**2 END DO END DO ! print*,'13 OK convect8' ! print*,'WA5 ',wa_moy DO l = 1, nlay DO ig = 1, ngrid pdtadj(ig, l) = zdhadj(ig, l)*zpspsk(ig, l) END DO END DO ! do l=1,nlay ! do ig=1,ngrid ! if(abs(pdtadj(ig,l))*86400..gt.500.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdtadj=',pdtadj(ig,l) ! endif ! if(abs(pdoadj(ig,l))*86400..gt.1.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdoadj=',pdoadj(ig,l) ! endif ! enddo ! enddo ! print*,'14 OK convect8' ! ------------------------------------------------------------------ ! Calculs pour les sorties ! ------------------------------------------------------------------ IF (sorties) THEN DO l = 1, nlay DO ig = 1, ngrid zla(ig, l) = (1.-fracd(ig,l))*zmax(ig) zld(ig, l) = fracd(ig, l)*zmax(ig) IF (1.-fracd(ig,l)>1.E-10) zwa(ig, l) = wd(ig, l)*fracd(ig, l)/ & (1.-fracd(ig,l)) END DO END DO DO l = 1, nlay DO ig = 1, ngrid detr(ig, l) = fm(ig, l) + entr(ig, l) - fm(ig, l+1) IF (detr(ig,l)<0.) THEN entr(ig, l) = entr(ig, l) - detr(ig, l) detr(ig, l) = 0. ! print*,'WARNING !!! detrainement negatif ',ig,l END IF END DO END DO END IF ! print*,'15 OK convect8' ! if(wa_moy(1,4).gt.1.e-10) stop ! print*,'19 OK convect8' RETURN END SUBROUTINE thermcell_2002 SUBROUTINE thermcell_cld(ngrid, nlay, ptimestep, pplay, pplev, pphi, zlev, & debut, pu, pv, pt, po, pduadj, pdvadj, pdtadj, pdoadj, fm0, entr0, zqla, & lmax, zmax_sec, wmax_sec, zw_sec, lmix_sec, ratqscth, ratqsdiff & ! s ! ,pu_therm,pv_therm , r_aspect, l_mix, w2di, tho) USE dimphy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! Réécriture à partir d'un listing papier à Habas, le 14/02/00 ! le thermique est supposé homogène et dissipé par mélange avec ! son environnement. la longueur l_mix contrôle l'efficacité du ! mélange ! Le calcul du transport des différentes espèces se fait en prenant ! en compte: ! 1. un flux de masse montant ! 2. un flux de masse descendant ! 3. un entrainement ! 4. un detrainement ! ======================================================================= ! ----------------------------------------------------------------------- ! declarations: ! ------------- include "dimensions.h" ! ccc#include "dimphy.h" include "YOMCST.h" include "YOETHF.h" include "FCTTRE.h" ! arguments: ! ---------- INTEGER ngrid, nlay, w2di REAL tho REAL ptimestep, l_mix, r_aspect REAL pt(ngrid, nlay), pdtadj(ngrid, nlay) REAL pu(ngrid, nlay), pduadj(ngrid, nlay) REAL pv(ngrid, nlay), pdvadj(ngrid, nlay) REAL po(ngrid, nlay), pdoadj(ngrid, nlay) REAL pplay(ngrid, nlay), pplev(ngrid, nlay+1) REAL pphi(ngrid, nlay) INTEGER idetr SAVE idetr DATA idetr/3/ !$OMP THREADPRIVATE(idetr) ! local: ! ------ INTEGER ig, k, l, lmaxa(klon), lmix(klon) REAL zsortie1d(klon) ! CR: on remplace lmax(klon,klev+1) INTEGER lmax(klon), lmin(klon), lentr(klon) REAL linter(klon) REAL zmix(klon), fracazmix(klon) REAL alpha SAVE alpha DATA alpha/1./ !$OMP THREADPRIVATE(alpha) ! RC REAL zmax(klon), zw, zz, zw2(klon, klev+1), ztva(klon, klev), zzz REAL zmax_sec(klon) REAL zmax_sec2(klon) REAL zw_sec(klon, klev+1) INTEGER lmix_sec(klon) REAL w_est(klon, klev+1) ! on garde le zmax du pas de temps precedent ! real zmax0(klon) ! save zmax0 ! real zmix0(klon) ! save zmix0 REAL, SAVE, ALLOCATABLE :: zmax0(:), zmix0(:) !$OMP THREADPRIVATE(zmax0, zmix0) REAL zlev(klon, klev+1), zlay(klon, klev) REAL deltaz(klon, klev) REAL zh(klon, klev), zdhadj(klon, klev) REAL zthl(klon, klev), zdthladj(klon, klev) REAL ztv(klon, klev) REAL zu(klon, klev), zv(klon, klev), zo(klon, klev) REAL zl(klon, klev) REAL wh(klon, klev+1) REAL wu(klon, klev+1), wv(klon, klev+1), wo(klon, klev+1) REAL zla(klon, klev+1) REAL zwa(klon, klev+1) REAL zld(klon, klev+1) REAL zwd(klon, klev+1) REAL zsortie(klon, klev) REAL zva(klon, klev) REAL zua(klon, klev) REAL zoa(klon, klev) REAL zta(klon, klev) REAL zha(klon, klev) REAL wa_moy(klon, klev+1) REAL fraca(klon, klev+1) REAL fracc(klon, klev+1) REAL zf, zf2 REAL thetath2(klon, klev), wth2(klon, klev), wth3(klon, klev) REAL q2(klon, klev) REAL dtheta(klon, klev) ! common/comtherm/thetath2,wth2 REAL ratqscth(klon, klev) REAL sum REAL sumdiff REAL ratqsdiff(klon, klev) REAL count_time INTEGER ialt LOGICAL sorties REAL rho(klon, klev), rhobarz(klon, klev+1), masse(klon, klev) REAL zpspsk(klon, klev) ! real wmax(klon,klev),wmaxa(klon) REAL wmax(klon), wmaxa(klon) REAL wmax_sec(klon) REAL wmax_sec2(klon) REAL wa(klon, klev, klev+1) REAL wd(klon, klev+1) REAL larg_part(klon, klev, klev+1) REAL fracd(klon, klev+1) REAL xxx(klon, klev+1) REAL larg_cons(klon, klev+1) REAL larg_detr(klon, klev+1) REAL fm0(klon, klev+1), entr0(klon, klev), detr(klon, klev) REAL massetot(klon, klev) REAL detr0(klon, klev) REAL alim0(klon, klev) REAL pu_therm(klon, klev), pv_therm(klon, klev) REAL fm(klon, klev+1), entr(klon, klev) REAL fmc(klon, klev+1) REAL zcor, zdelta, zcvm5, qlbef REAL tbef(klon), qsatbef(klon) REAL dqsat_dt, dt, num, denom REAL reps, rlvcp, ddt0 REAL ztla(klon, klev), zqla(klon, klev), zqta(klon, klev) ! CR niveau de condensation REAL nivcon(klon) REAL zcon(klon) REAL zqsat(klon, klev) REAL zqsatth(klon, klev) PARAMETER (ddt0=.01) ! CR:nouvelles variables REAL f_star(klon, klev+1), entr_star(klon, klev) REAL detr_star(klon, klev) REAL alim_star_tot(klon), alim_star2(klon) REAL entr_star_tot(klon) REAL detr_star_tot(klon) REAL alim_star(klon, klev) REAL alim(klon, klev) REAL nu(klon, klev) REAL nu_e(klon, klev) REAL nu_min REAL nu_max REAL nu_r REAL f(klon) ! real f(klon), f0(klon) ! save f0 REAL, SAVE, ALLOCATABLE :: f0(:) !$OMP THREADPRIVATE(f0) REAL f_old REAL zlevinter(klon) LOGICAL, SAVE :: first = .TRUE. !$OMP THREADPRIVATE(first) ! data first /.false./ ! save first LOGICAL nuage ! save nuage LOGICAL boucle LOGICAL therm LOGICAL debut LOGICAL rale INTEGER test(klon) INTEGER signe_zw2 ! RC CHARACTER *2 str2 CHARACTER *10 str10 CHARACTER (LEN=20) :: modname = 'thermcell_cld' CHARACTER (LEN=80) :: abort_message LOGICAL vtest(klon), down LOGICAL zsat(klon) EXTERNAL scopy INTEGER ncorrec, ll SAVE ncorrec DATA ncorrec/0/ !$OMP THREADPRIVATE(ncorrec) ! ----------------------------------------------------------------------- ! initialisation: ! --------------- IF (first) THEN ALLOCATE (zmix0(klon)) ALLOCATE (zmax0(klon)) ALLOCATE (f0(klon)) first = .FALSE. END IF sorties = .FALSE. ! print*,'NOUVEAU DETR PLUIE ' IF (ngrid/=klon) THEN PRINT * PRINT *, 'STOP dans convadj' PRINT *, 'ngrid =', ngrid PRINT *, 'klon =', klon END IF ! Initialisation rlvcp = rlvtt/rcpd reps = rd/rv ! initialisations de zqsat DO ll = 1, nlay DO ig = 1, ngrid zqsat(ig, ll) = 0. zqsatth(ig, ll) = 0. END DO END DO ! on met le first a true pour le premier passage de la journée DO ig = 1, klon test(ig) = 0 END DO IF (debut) THEN DO ig = 1, klon test(ig) = 1 f0(ig) = 0. zmax0(ig) = 0. END DO END IF DO ig = 1, klon IF ((.NOT. debut) .AND. (f0(ig)<1.E-10)) THEN test(ig) = 1 END IF END DO ! do ig=1,klon ! print*,'test(ig)',test(ig),zmax0(ig) ! enddo nuage = .FALSE. ! ----------------------------------------------------------------------- ! AM Calcul de T,q,ql a partir de Tl et qT ! --------------------------------------------------- ! Pr Tprec=Tl calcul de qsat ! Si qsat>qT T=Tl, q=qT ! Sinon DDT=(-Tprec+Tl+RLVCP (qT-qsat(T')) / (1+RLVCP dqsat/dt) ! On cherche DDT < DDT0 ! defaut DO ll = 1, nlay DO ig = 1, ngrid zo(ig, ll) = po(ig, ll) zl(ig, ll) = 0. zh(ig, ll) = pt(ig, ll) END DO END DO DO ig = 1, ngrid zsat(ig) = .FALSE. END DO DO ll = 1, nlay ! les points insatures sont definitifs DO ig = 1, ngrid tbef(ig) = pt(ig, ll) zdelta = max(0., sign(1.,rtt-tbef(ig))) qsatbef(ig) = r2es*foeew(tbef(ig), zdelta)/pplev(ig, ll) qsatbef(ig) = min(0.5, qsatbef(ig)) zcor = 1./(1.-retv*qsatbef(ig)) qsatbef(ig) = qsatbef(ig)*zcor zsat(ig) = (max(0.,po(ig,ll)-qsatbef(ig))>1.E-10) END DO DO ig = 1, ngrid IF (zsat(ig) .AND. (1==1)) THEN qlbef = max(0., po(ig,ll)-qsatbef(ig)) ! si sature: ql est surestime, d'ou la sous-relax dt = 0.5*rlvcp*qlbef ! write(18,*),'DT0=',DT ! on pourra enchainer 2 ou 3 calculs sans Do while DO WHILE (abs(dt)>ddt0) ! il faut verifier si c,a conserve quand on repasse en insature ... tbef(ig) = tbef(ig) + dt zdelta = max(0., sign(1.,rtt-tbef(ig))) qsatbef(ig) = r2es*foeew(tbef(ig), zdelta)/pplev(ig, ll) qsatbef(ig) = min(0.5, qsatbef(ig)) zcor = 1./(1.-retv*qsatbef(ig)) qsatbef(ig) = qsatbef(ig)*zcor ! on veut le signe de qlbef qlbef = po(ig, ll) - qsatbef(ig) zdelta = max(0., sign(1.,rtt-tbef(ig))) zcvm5 = r5les*(1.-zdelta) + r5ies*zdelta zcor = 1./(1.-retv*qsatbef(ig)) dqsat_dt = foede(tbef(ig), zdelta, zcvm5, qsatbef(ig), zcor) num = -tbef(ig) + pt(ig, ll) + rlvcp*qlbef denom = 1. + rlvcp*dqsat_dt IF (denom<1.E-10) THEN PRINT *, 'pb denom' END IF dt = num/denom END DO ! on ecrit de maniere conservative (sat ou non) zl(ig, ll) = max(0., qlbef) ! T = Tl +Lv/Cp ql zh(ig, ll) = pt(ig, ll) + rlvcp*zl(ig, ll) zo(ig, ll) = po(ig, ll) - zl(ig, ll) END IF ! on ecrit zqsat zqsat(ig, ll) = qsatbef(ig) END DO END DO ! AM fin ! ----------------------------------------------------------------------- ! incrementation eventuelle de tendances precedentes: ! --------------------------------------------------- ! print*,'0 OK convect8' DO l = 1, nlay DO ig = 1, ngrid zpspsk(ig, l) = (pplay(ig,l)/100000.)**rkappa ! zpspsk(ig,l)=(pplay(ig,l)/pplev(ig,1))**RKAPPA ! zh(ig,l)=pt(ig,l)/zpspsk(ig,l) zu(ig, l) = pu(ig, l) zv(ig, l) = pv(ig, l) ! zo(ig,l)=po(ig,l) ! ztv(ig,l)=zh(ig,l)*(1.+0.61*zo(ig,l)) ! AM attention zh est maintenant le profil de T et plus le profil de ! theta ! ! T-> Theta ztv(ig, l) = zh(ig, l)/zpspsk(ig, l) ! AM Theta_v ztv(ig, l) = ztv(ig, l)*(1.+retv*(zo(ig,l))-zl(ig,l)) ! AM Thetal zthl(ig, l) = pt(ig, l)/zpspsk(ig, l) END DO END DO ! print*,'1 OK convect8' ! -------------------- ! + + + + + + + + + + + ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz ! wh,wt,wo ... ! + + + + + + + + + + + zh,zu,zv,zo,rho ! -------------------- zlev(1) ! \\\\\\\\\\\\\\\\\\\\ ! ----------------------------------------------------------------------- ! Calcul des altitudes des couches ! ----------------------------------------------------------------------- DO l = 2, nlay DO ig = 1, ngrid zlev(ig, l) = 0.5*(pphi(ig,l)+pphi(ig,l-1))/rg END DO END DO DO ig = 1, ngrid zlev(ig, 1) = 0. zlev(ig, nlay+1) = (2.*pphi(ig,klev)-pphi(ig,klev-1))/rg END DO DO l = 1, nlay DO ig = 1, ngrid zlay(ig, l) = pphi(ig, l)/rg END DO END DO ! calcul de deltaz DO l = 1, nlay DO ig = 1, ngrid deltaz(ig, l) = zlev(ig, l+1) - zlev(ig, l) END DO END DO ! print*,'2 OK convect8' ! ----------------------------------------------------------------------- ! Calcul des densites ! ----------------------------------------------------------------------- DO l = 1, nlay DO ig = 1, ngrid ! rho(ig,l)=pplay(ig,l)/(zpspsk(ig,l)*RD*zh(ig,l)) rho(ig, l) = pplay(ig, l)/(zpspsk(ig,l)*rd*ztv(ig,l)) END DO END DO DO l = 2, nlay DO ig = 1, ngrid rhobarz(ig, l) = 0.5*(rho(ig,l)+rho(ig,l-1)) END DO END DO DO k = 1, nlay DO l = 1, nlay + 1 DO ig = 1, ngrid wa(ig, k, l) = 0. END DO END DO END DO ! Cr:ajout:calcul de la masse DO l = 1, nlay DO ig = 1, ngrid ! masse(ig,l)=rho(ig,l)*(zlev(ig,l+1)-zlev(ig,l)) masse(ig, l) = (pplev(ig,l)-pplev(ig,l+1))/rg END DO END DO ! print*,'3 OK convect8' ! ------------------------------------------------------------------ ! Calcul de w2, quarre de w a partir de la cape ! a partir de w2, on calcule wa, vitesse de l'ascendance ! ATTENTION: Dans cette version, pour cause d'economie de memoire, ! w2 est stoke dans wa ! ATTENTION: dans convect8, on n'utilise le calcule des wa ! independants par couches que pour calculer l'entrainement ! a la base et la hauteur max de l'ascendance. ! Indicages: ! l'ascendance provenant du niveau k traverse l'interface l avec ! une vitesse wa(k,l). ! -------------------- ! + + + + + + + + + + ! wa(k,l) ---- -------------------- l ! /\ ! /||\ + + + + + + + + + + ! || ! || -------------------- ! || ! || + + + + + + + + + + ! || ! || -------------------- ! ||__ ! |___ + + + + + + + + + + k ! -------------------- ! ------------------------------------------------------------------ ! CR: ponderation entrainement des couches instables ! def des alim_star tels que alim=f*alim_star DO l = 1, klev DO ig = 1, ngrid alim_star(ig, l) = 0. alim(ig, l) = 0. END DO END DO ! determination de la longueur de la couche d entrainement DO ig = 1, ngrid lentr(ig) = 1 END DO ! on ne considere que les premieres couches instables therm = .FALSE. DO k = nlay - 2, 1, -1 DO ig = 1, ngrid IF (ztv(ig,k)>ztv(ig,k+1) .AND. ztv(ig,k+1)<=ztv(ig,k+2)) THEN lentr(ig) = k + 1 therm = .TRUE. END IF END DO END DO ! determination du lmin: couche d ou provient le thermique DO ig = 1, ngrid lmin(ig) = 1 END DO DO ig = 1, ngrid DO l = nlay, 2, -1 IF (ztv(ig,l-1)>ztv(ig,l)) THEN lmin(ig) = l - 1 END IF END DO END DO ! definition de l'entrainement des couches DO l = 1, klev - 1 DO ig = 1, ngrid IF (ztv(ig,l)>ztv(ig,l+1) .AND. l>=lmin(ig) .AND. l1.E-10) THEN ! do l=1,lentr(ig) DO l = 1, klev ! def possibles pour entr_star: zdthetadz, dthetadz, zdtheta alim_star(ig, l) = alim_star(ig, l)/alim_star_tot(ig) END DO END IF END DO ! print*,'fin calcul alim_star' ! AM:initialisations DO k = 1, nlay DO ig = 1, ngrid ztva(ig, k) = ztv(ig, k) ztla(ig, k) = zthl(ig, k) zqla(ig, k) = 0. zqta(ig, k) = po(ig, k) zsat(ig) = .FALSE. END DO END DO DO k = 1, klev DO ig = 1, ngrid detr_star(ig, k) = 0. entr_star(ig, k) = 0. detr(ig, k) = 0. entr(ig, k) = 0. END DO END DO ! print*,'7 OK convect8' DO k = 1, klev + 1 DO ig = 1, ngrid zw2(ig, k) = 0. fmc(ig, k) = 0. ! CR f_star(ig, k) = 0. ! RC larg_cons(ig, k) = 0. larg_detr(ig, k) = 0. wa_moy(ig, k) = 0. END DO END DO ! n print*,'8 OK convect8' DO ig = 1, ngrid linter(ig) = 1. lmaxa(ig) = 1 lmix(ig) = 1 wmaxa(ig) = 0. END DO nu_min = l_mix nu_max = 1000. ! do ig=1,ngrid ! nu_max=wmax_sec(ig) ! enddo DO ig = 1, ngrid DO k = 1, klev nu(ig, k) = 0. nu_e(ig, k) = 0. END DO END DO ! Calcul de l'excès de température du à la diffusion turbulente DO ig = 1, ngrid DO l = 1, klev dtheta(ig, l) = 0. END DO END DO DO ig = 1, ngrid DO l = 1, lentr(ig) - 1 dtheta(ig, l) = sqrt(10.*0.4*zlev(ig,l+1)**2*1.*((ztv(ig,l+1)- & ztv(ig,l))/(zlev(ig,l+1)-zlev(ig,l)))**2) END DO END DO ! do l=1,nlay-2 DO l = 1, klev - 1 DO ig = 1, ngrid IF (ztv(ig,l)>ztv(ig,l+1) .AND. alim_star(ig,l)>1.E-10 .AND. & zw2(ig,l)<1E-10) THEN ! AM ! test:on rajoute un excès de T dans couche alim ! ztla(ig,l)=zthl(ig,l)+dtheta(ig,l) ztla(ig, l) = zthl(ig, l) ! test: on rajoute un excès de q dans la couche alim ! zqta(ig,l)=po(ig,l)+0.001 zqta(ig, l) = po(ig, l) zqla(ig, l) = zl(ig, l) ! AM f_star(ig, l+1) = alim_star(ig, l) ! test:calcul de dteta zw2(ig, l+1) = 2.*rg*(ztv(ig,l)-ztv(ig,l+1))/ztv(ig, l+1)* & (zlev(ig,l+1)-zlev(ig,l))*0.4*pphi(ig, l)/(pphi(ig,l+1)-pphi(ig,l)) w_est(ig, l+1) = zw2(ig, l+1) larg_detr(ig, l) = 0. ! print*,'coucou boucle 1' ELSE IF ((zw2(ig,l)>=1E-10) .AND. (f_star(ig,l)+alim_star(ig, & l))>1.E-10) THEN ! print*,'coucou boucle 2' ! estimation du detrainement a partir de la geometrie du pas ! precedent IF ((test(ig)==1) .OR. ((.NOT. debut) .AND. (f0(ig)<1.E-10))) THEN detr_star(ig, l) = 0. entr_star(ig, l) = 0. ! print*,'coucou test(ig)',test(ig),f0(ig),zmax0(ig) ELSE ! print*,'coucou debut detr' ! tests sur la definition du detr IF (zqla(ig,l-1)>1.E-10) THEN nuage = .TRUE. END IF w_est(ig, l+1) = zw2(ig, l)*((f_star(ig,l))**2)/(f_star(ig,l)+ & alim_star(ig,l))**2 + 2.*rg*(ztva(ig,l-1)-ztv(ig,l))/ztv(ig, l)*( & zlev(ig,l+1)-zlev(ig,l)) IF (w_est(ig,l+1)<0.) THEN w_est(ig, l+1) = zw2(ig, l) END IF IF (l>2) THEN IF ((w_est(ig,l+1)>w_est(ig,l)) .AND. (zlev(ig, & l+1)f_star(ig,l)) THEN detr_star(ig, l) = f_star(ig, l) ! entr_star(ig,l)=0. END IF IF ((l1.E-10) THEN ! then ! test ! if (((f_star(ig,l+1)+detr_star(ig,l)).gt.1.e-10)) then ! AM on melange Tl et qt du thermique ! on rajoute un excès de T dans la couche alim ! if (l.lt.lentr(ig)) then ! ztla(ig,l)=(f_star(ig,l)*ztla(ig,l-1)+ ! s ! (alim_star(ig,l)+entr_star(ig,l))*(zthl(ig,l)+dtheta(ig,l))) ! s /(f_star(ig,l+1)+detr_star(ig,l)) ! else ztla(ig, l) = (f_star(ig,l)*ztla(ig,l-1)+(alim_star(ig, & l)+entr_star(ig,l))*zthl(ig,l))/(f_star(ig,l+1)+detr_star(ig,l)) ! s /(f_star(ig,l+1)) ! endif ! on rajoute un excès de q dans la couche alim ! if (l.lt.lentr(ig)) then ! zqta(ig,l)=(f_star(ig,l)*zqta(ig,l-1)+ ! s (alim_star(ig,l)+entr_star(ig,l))*(po(ig,l)+0.001)) ! s /(f_star(ig,l+1)+detr_star(ig,l)) ! else zqta(ig, l) = (f_star(ig,l)*zqta(ig,l-1)+(alim_star(ig, & l)+entr_star(ig,l))*po(ig,l))/(f_star(ig,l+1)+detr_star(ig,l)) ! s /(f_star(ig,l+1)) ! endif ! AM on en deduit thetav et ql du thermique ! CR test ! Tbef(ig)=ztla(ig,l)*zpspsk(ig,l) tbef(ig) = ztla(ig, l)*zpspsk(ig, l) zdelta = max(0., sign(1.,rtt-tbef(ig))) qsatbef(ig) = r2es*foeew(tbef(ig), zdelta)/pplev(ig, l) qsatbef(ig) = min(0.5, qsatbef(ig)) zcor = 1./(1.-retv*qsatbef(ig)) qsatbef(ig) = qsatbef(ig)*zcor zsat(ig) = (max(0.,zqta(ig,l)-qsatbef(ig))>1.E-10) IF (zsat(ig) .AND. (1==1)) THEN qlbef = max(0., zqta(ig,l)-qsatbef(ig)) dt = 0.5*rlvcp*qlbef ! write(17,*)'DT0=',DT DO WHILE (abs(dt)>ddt0) ! print*,'aie' tbef(ig) = tbef(ig) + dt zdelta = max(0., sign(1.,rtt-tbef(ig))) qsatbef(ig) = r2es*foeew(tbef(ig), zdelta)/pplev(ig, l) qsatbef(ig) = min(0.5, qsatbef(ig)) zcor = 1./(1.-retv*qsatbef(ig)) qsatbef(ig) = qsatbef(ig)*zcor qlbef = zqta(ig, l) - qsatbef(ig) zdelta = max(0., sign(1.,rtt-tbef(ig))) zcvm5 = r5les*(1.-zdelta) + r5ies*zdelta zcor = 1./(1.-retv*qsatbef(ig)) dqsat_dt = foede(tbef(ig), zdelta, zcvm5, qsatbef(ig), zcor) num = -tbef(ig) + ztla(ig, l)*zpspsk(ig, l) + rlvcp*qlbef denom = 1. + rlvcp*dqsat_dt IF (denom<1.E-10) THEN PRINT *, 'pb denom' END IF dt = num/denom ! write(17,*)'DT=',DT END DO zqla(ig, l) = max(0., zqta(ig,l)-qsatbef(ig)) zqla(ig, l) = max(0., qlbef) ! zqla(ig,l)=0. END IF ! zqla(ig,l) = max(0.,zqta(ig,l)-qsatbef(ig)) ! on ecrit de maniere conservative (sat ou non) ! T = Tl +Lv/Cp ql ! CR rq utilisation de humidite specifique ou rapport de melange? ztva(ig, l) = ztla(ig, l)*zpspsk(ig, l) + rlvcp*zqla(ig, l) ztva(ig, l) = ztva(ig, l)/zpspsk(ig, l) ! on rajoute le calcul de zha pour diagnostiques (temp potentielle) zha(ig, l) = ztva(ig, l) ! if (l.lt.lentr(ig)) then ! ztva(ig,l) = ztva(ig,l)*(1.+RETV*(zqta(ig,l) ! s -zqla(ig,l))-zqla(ig,l)) + 0.1 ! else ztva(ig, l) = ztva(ig, l)*(1.+retv*(zqta(ig,l)-zqla(ig, & l))-zqla(ig,l)) ! endif ! ztva(ig,l) = ztla(ig,l)*zpspsk(ig,l)+RLvCp*zqla(ig,l) ! s /(1.-retv*zqla(ig,l)) ! ztva(ig,l) = ztva(ig,l)/zpspsk(ig,l) ! ztva(ig,l) = ztva(ig,l)*(1.+RETV*(zqta(ig,l) ! s /(1.-retv*zqta(ig,l)) ! s -zqla(ig,l)/(1.-retv*zqla(ig,l))) ! s -zqla(ig,l)/(1.-retv*zqla(ig,l))) ! write(13,*)zqla(ig,l),zqla(ig,l)/(1.-retv*zqla(ig,l)) ! on ecrit zqsat zqsatth(ig, l) = qsatbef(ig) ! enddo ! DO ig=1,ngrid ! if (zw2(ig,l).ge.1.e-10.and. ! s f_star(ig,l)+entr_star(ig,l).gt.1.e-10) then ! mise a jour de la vitesse ascendante (l'air entraine de la couche ! consideree commence avec une vitesse nulle). ! if (f_star(ig,l+1).gt.1.e-10) then zw2(ig, l+1) = zw2(ig, l)* & ! s ! ((f_star(ig,l)-detr_star(ig,l))**2) ! s /f_star(ig,l+1)**2+ ((f_star(ig,l))**2)/(f_star(ig,l+1)+detr_star(ig,l))**2 + & ! s ! /(f_star(ig,l+1))**2+ 2.*rg*(ztva(ig,l)-ztv(ig,l))/ztv(ig, l)*(zlev(ig,l+1)-zlev(ig,l)) ! s *(f_star(ig,l)/f_star(ig,l+1))**2 END IF END IF IF (zw2(ig,l+1)<0.) THEN linter(ig) = (l*(zw2(ig,l+1)-zw2(ig,l))-zw2(ig,l))/(zw2(ig,l+1)-zw2( & ig,l)) zw2(ig, l+1) = 0. ! print*,'linter=',linter(ig) ! else if ((zw2(ig,l+1).lt.1.e-10).and.(zw2(ig,l+1).ge.0.)) then ! linter(ig)=l+1 ! print*,'linter=l',zw2(ig,l),zw2(ig,l+1) ELSE wa_moy(ig, l+1) = sqrt(zw2(ig,l+1)) ! wa_moy(ig,l+1)=zw2(ig,l+1) END IF IF (wa_moy(ig,l+1)>wmaxa(ig)) THEN ! lmix est le niveau de la couche ou w (wa_moy) est maximum lmix(ig) = l + 1 wmaxa(ig) = wa_moy(ig, l+1) END IF END DO END DO PRINT *, 'fin calcul zw2' ! Calcul de la couche correspondant a la hauteur du thermique DO ig = 1, ngrid lmax(ig) = lentr(ig) END DO DO ig = 1, ngrid DO l = nlay, lentr(ig) + 1, -1 IF (zw2(ig,l)<=1.E-10) THEN lmax(ig) = l - 1 END IF END DO END DO ! pas de thermique si couche 1 stable DO ig = 1, ngrid IF (lmin(ig)>1) THEN lmax(ig) = 1 lmin(ig) = 1 lentr(ig) = 1 END IF END DO ! Determination de zw2 max DO ig = 1, ngrid wmax(ig) = 0. END DO DO l = 1, nlay DO ig = 1, ngrid IF (l<=lmax(ig)) THEN IF (zw2(ig,l)<0.) THEN PRINT *, 'pb2 zw2<0' END IF zw2(ig, l) = sqrt(zw2(ig,l)) wmax(ig) = max(wmax(ig), zw2(ig,l)) ELSE zw2(ig, l) = 0. END IF END DO END DO ! Longueur caracteristique correspondant a la hauteur des thermiques. DO ig = 1, ngrid zmax(ig) = 0. zlevinter(ig) = zlev(ig, 1) END DO DO ig = 1, ngrid ! calcul de zlevinter zlevinter(ig) = (zlev(ig,lmax(ig)+1)-zlev(ig,lmax(ig)))*linter(ig) + & zlev(ig, lmax(ig)) - lmax(ig)*(zlev(ig,lmax(ig)+1)-zlev(ig,lmax(ig))) ! pour le cas ou on prend tjs lmin=1 ! zmax(ig)=max(zmax(ig),zlevinter(ig)-zlev(ig,lmin(ig))) zmax(ig) = max(zmax(ig), zlevinter(ig)-zlev(ig,1)) zmax0(ig) = zmax(ig) WRITE (11, *) 'ig,lmax,linter', ig, lmax(ig), linter(ig) WRITE (12, *) 'ig,zlevinter,zmax', ig, zmax(ig), zlevinter(ig) END DO ! Calcul de zmax_sec et wmax_sec CALL fermeture_seche(ngrid, nlay, pplay, pplev, pphi, zlev, rhobarz, f0, & zpspsk, alim, zh, zo, lentr, lmin, nu_min, nu_max, r_aspect, zmax_sec2, & wmax_sec2) PRINT *, 'avant fermeture' ! Fermeture,determination de f ! en lmax f=d-e DO ig = 1, ngrid ! entr_star(ig,lmax(ig))=0. ! f_star(ig,lmax(ig)+1)=0. ! detr_star(ig,lmax(ig))=f_star(ig,lmax(ig))+entr_star(ig,lmax(ig)) ! s +alim_star(ig,lmax(ig)) END DO DO ig = 1, ngrid alim_star2(ig) = 0. END DO ! calcul de entr_star_tot DO ig = 1, ngrid DO k = 1, lmix(ig) entr_star_tot(ig) = entr_star_tot(ig) & ! s ! +entr_star(ig,k) +alim_star(ig, k) ! s -detr_star(ig,k) detr_star_tot(ig) = detr_star_tot(ig) & ! s ! +alim_star(ig,k) -detr_star(ig, k) + entr_star(ig, k) END DO END DO DO ig = 1, ngrid IF (alim_star_tot(ig)<1.E-10) THEN f(ig) = 0. ELSE ! do k=lmin(ig),lentr(ig) DO k = 1, lentr(ig) alim_star2(ig) = alim_star2(ig) + alim_star(ig, k)**2/(rho(ig,k)*( & zlev(ig,k+1)-zlev(ig,k))) END DO IF ((zmax_sec(ig)>1.E-10) .AND. (1==1)) THEN f(ig) = wmax_sec(ig)/(max(500.,zmax_sec(ig))*r_aspect*alim_star2(ig)) f(ig) = f(ig) + (f0(ig)-f(ig))*exp((-ptimestep/zmax_sec(ig))*wmax_sec & (ig)) ELSE f(ig) = wmax(ig)/(max(500.,zmax(ig))*r_aspect*alim_star2(ig)) f(ig) = f(ig) + (f0(ig)-f(ig))*exp((-ptimestep/zmax(ig))*wmax(ig)) END IF END IF f0(ig) = f(ig) END DO PRINT *, 'apres fermeture' ! Calcul de l'entrainement DO ig = 1, ngrid DO k = 1, klev alim(ig, k) = f(ig)*alim_star(ig, k) END DO END DO ! CR:test pour entrainer moins que la masse ! do ig=1,ngrid ! do l=1,lentr(ig) ! if ((alim(ig,l)*ptimestep).gt.(0.9*masse(ig,l))) then ! alim(ig,l+1)=alim(ig,l+1)+alim(ig,l) ! s -0.9*masse(ig,l)/ptimestep ! alim(ig,l)=0.9*masse(ig,l)/ptimestep ! endif ! enddo ! enddo ! calcul du détrainement DO ig = 1, klon DO k = 1, klev detr(ig, k) = f(ig)*detr_star(ig, k) IF (detr(ig,k)<0.) THEN ! print*,'detr1<0!!!' END IF END DO DO k = 1, klev entr(ig, k) = f(ig)*entr_star(ig, k) IF (entr(ig,k)<0.) THEN ! print*,'entr1<0!!!' END IF END DO END DO ! do ig=1,ngrid ! do l=1,klev ! if (((detr(ig,l)+entr(ig,l)+alim(ig,l))*ptimestep).gt. ! s (masse(ig,l))) then ! print*,'d2+e2+a2>m2','ig=',ig,'l=',l,'lmax(ig)=',lmax(ig),'d+e+a=' ! s,(detr(ig,l)+entr(ig,l)+alim(ig,l))*ptimestep,'m=',masse(ig,l) ! endif ! enddo ! enddo ! Calcul des flux DO ig = 1, ngrid DO l = 1, lmax(ig) ! do l=1,klev ! fmc(ig,l+1)=f(ig)*f_star(ig,l+1) fmc(ig, l+1) = fmc(ig, l) + alim(ig, l) + entr(ig, l) - detr(ig, l) ! print*,'??!!','ig=',ig,'l=',l,'lmax=',lmax(ig),'lmix=',lmix(ig), ! s 'e=',entr(ig,l),'d=',detr(ig,l),'a=',alim(ig,l),'f=',fmc(ig,l), ! s 'f+1=',fmc(ig,l+1) IF (fmc(ig,l+1)<0.) THEN PRINT *, 'fmc1<0', l + 1, lmax(ig), fmc(ig, l+1) fmc(ig, l+1) = fmc(ig, l) detr(ig, l) = alim(ig, l) + entr(ig, l) ! fmc(ig,l+1)=0. ! print*,'fmc1<0',l+1,lmax(ig),fmc(ig,l+1) END IF ! if ((fmc(ig,l+1).gt.fmc(ig,l)).and.(l.gt.lentr(ig))) then ! f_old=fmc(ig,l+1) ! fmc(ig,l+1)=fmc(ig,l) ! detr(ig,l)=detr(ig,l)+f_old-fmc(ig,l+1) ! endif ! if ((fmc(ig,l+1).gt.fmc(ig,l)).and.(l.gt.lentr(ig))) then ! f_old=fmc(ig,l+1) ! fmc(ig,l+1)=fmc(ig,l) ! detr(ig,l)=detr(ig,l)+f_old-fmc(ig,l) ! endif ! rajout du test sur alpha croissant ! if test ! if (1.eq.0) then IF (l==klev) THEN PRINT *, 'THERMCELL PB ig=', ig, ' l=', l abort_message = 'THERMCELL PB' CALL abort_physic(modname, abort_message, 1) END IF ! if ((zw2(ig,l+1).gt.1.e-10).and.(zw2(ig,l).gt.1.e-10).and. ! s (l.ge.lentr(ig)).and. IF ((zw2(ig,l+1)>1.E-10) .AND. (zw2(ig,l)>1.E-10) .AND. (l>=lentr(ig))) & THEN IF (((fmc(ig,l+1)/(rhobarz(ig,l+1)*zw2(ig,l+1)))>(fmc(ig,l)/ & (rhobarz(ig,l)*zw2(ig,l))))) THEN f_old = fmc(ig, l+1) fmc(ig, l+1) = fmc(ig, l)*rhobarz(ig, l+1)*zw2(ig, l+1)/ & (rhobarz(ig,l)*zw2(ig,l)) detr(ig, l) = detr(ig, l) + f_old - fmc(ig, l+1) ! detr(ig,l)=(fmc(ig,l+1)-fmc(ig,l))/(0.4-1.) ! entr(ig,l)=0.4*detr(ig,l) ! entr(ig,l)=fmc(ig,l+1)-fmc(ig,l)+detr(ig,l) END IF END IF IF ((fmc(ig,l+1)>fmc(ig,l)) .AND. (l>lentr(ig))) THEN f_old = fmc(ig, l+1) fmc(ig, l+1) = fmc(ig, l) detr(ig, l) = detr(ig, l) + f_old - fmc(ig, l+1) END IF IF (detr(ig,l)>fmc(ig,l)) THEN detr(ig, l) = fmc(ig, l) entr(ig, l) = fmc(ig, l+1) - alim(ig, l) END IF IF (fmc(ig,l+1)<0.) THEN detr(ig, l) = detr(ig, l) + fmc(ig, l+1) fmc(ig, l+1) = 0. PRINT *, 'fmc2<0', l + 1, lmax(ig) END IF ! test pour ne pas avoir f=0 et d=e/=0 ! if (fmc(ig,l+1).lt.1.e-10) then ! detr(ig,l+1)=0. ! entr(ig,l+1)=0. ! zqla(ig,l+1)=0. ! zw2(ig,l+1)=0. ! lmax(ig)=l+1 ! zmax(ig)=zlev(ig,lmax(ig)) ! endif IF (zw2(ig,l+1)>1.E-10) THEN IF ((((fmc(ig,l+1))/(rhobarz(ig,l+1)*zw2(ig,l+1)))>1.)) THEN f_old = fmc(ig, l+1) fmc(ig, l+1) = rhobarz(ig, l+1)*zw2(ig, l+1) zw2(ig, l+1) = 0. zqla(ig, l+1) = 0. detr(ig, l) = detr(ig, l) + f_old - fmc(ig, l+1) lmax(ig) = l + 1 zmax(ig) = zlev(ig, lmax(ig)) PRINT *, 'alpha>1', l + 1, lmax(ig) END IF END IF ! write(1,*)'ig,l,fm(ig,l)',ig,l,fm(ig,l) ! endif test ! endif END DO END DO DO ig = 1, ngrid ! if (fmc(ig,lmax(ig)+1).ne.0.) then fmc(ig, lmax(ig)+1) = 0. entr(ig, lmax(ig)) = 0. detr(ig, lmax(ig)) = fmc(ig, lmax(ig)) + entr(ig, lmax(ig)) + & alim(ig, lmax(ig)) ! endif END DO ! test sur le signe de fmc DO ig = 1, ngrid DO l = 1, klev + 1 IF (fmc(ig,l)<0.) THEN PRINT *, 'fm1<0!!!', 'ig=', ig, 'l=', l, 'a=', alim(ig, l-1), 'e=', & entr(ig, l-1), 'f=', fmc(ig, l-1), 'd=', detr(ig, l-1), 'f+1=', & fmc(ig, l) END IF END DO END DO ! test de verification DO ig = 1, ngrid DO l = 1, lmax(ig) IF ((abs(fmc(ig,l+1)-fmc(ig,l)-alim(ig,l)-entr(ig,l)+ & detr(ig,l)))>1.E-4) THEN ! print*,'pbcm!!','ig=',ig,'l=',l,'lmax=',lmax(ig),'lmix=',lmix(ig), ! s 'e=',entr(ig,l),'d=',detr(ig,l),'a=',alim(ig,l),'f=',fmc(ig,l), ! s 'f+1=',fmc(ig,l+1) END IF IF (detr(ig,l)<0.) THEN PRINT *, 'detrdemi<0!!!' END IF END DO END DO ! RC ! CR def de zmix continu (profil parabolique des vitesses) DO ig = 1, ngrid IF (lmix(ig)>1.) THEN ! test IF (((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)))- & (zlev(ig,lmix(ig)+1)))-(zw2(ig,lmix(ig))- & zw2(ig,lmix(ig)+1))*((zlev(ig,lmix(ig)-1))- & (zlev(ig,lmix(ig)))))>1E-10) THEN zmix(ig) = ((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)) & )**2-(zlev(ig,lmix(ig)+1))**2)-(zw2(ig,lmix(ig))-zw2(ig, & lmix(ig)+1))*((zlev(ig,lmix(ig)-1))**2-(zlev(ig,lmix(ig)))**2))/ & (2.*((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)))- & (zlev(ig,lmix(ig)+1)))-(zw2(ig,lmix(ig))- & zw2(ig,lmix(ig)+1))*((zlev(ig,lmix(ig)-1))-(zlev(ig,lmix(ig)))))) ELSE zmix(ig) = zlev(ig, lmix(ig)) PRINT *, 'pb zmix' END IF ELSE zmix(ig) = 0. END IF ! test IF ((zmax(ig)-zmix(ig))<=0.) THEN zmix(ig) = 0.9*zmax(ig) ! print*,'pb zmix>zmax' END IF END DO DO ig = 1, klon zmix0(ig) = zmix(ig) END DO ! calcul du nouveau lmix correspondant DO ig = 1, ngrid DO l = 1, klev IF (zmix(ig)>=zlev(ig,l) .AND. zmix(ig)(fmc(ig,l)+alim(ig,l))+entr(ig,l)) THEN PRINT *, 'detr2>fmc2!!!', 'ig=', ig, 'l=', l, 'd=', detr(ig, l), & 'f=', fmc(ig, l), 'lmax=', lmax(ig) ! detr(ig,l)=fmc(ig,l)+alim(ig,l)+entr(ig,l) ! entr(ig,l)=0. ! fmc(ig,l+1)=0. ! zw2(ig,l+1)=0. ! zqla(ig,l+1)=0. PRINT *, 'pb!fm=0 et f_star>0', l, lmax(ig) ! lmax(ig)=l END IF END DO END DO DO ig = 1, ngrid DO l = lmax(ig) + 1, klev + 1 ! fmc(ig,l)=0. ! detr(ig,l)=0. ! entr(ig,l)=0. ! zw2(ig,l)=0. ! zqla(ig,l)=0. END DO END DO ! Calcul du detrainement lors du premier passage ! print*,'9 OK convect8' ! print*,'WA1 ',wa_moy ! determination de l'indice du debut de la mixed layer ou w decroit ! calcul de la largeur de chaque ascendance dans le cas conservatif. ! dans ce cas simple, on suppose que la largeur de l'ascendance provenant ! d'une couche est égale à la hauteur de la couche alimentante. ! La vitesse maximale dans l'ascendance est aussi prise comme estimation ! de la vitesse d'entrainement horizontal dans la couche alimentante. DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmax(ig) .AND. (test(ig)==1)) THEN zw = max(wa_moy(ig,l), 1.E-10) larg_cons(ig, l) = zmax(ig)*r_aspect*fmc(ig, l)/(rhobarz(ig,l)*zw) END IF END DO END DO DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmax(ig) .AND. (test(ig)==1)) THEN ! if (idetr.eq.0) then ! cette option est finalement en dur. IF ((l_mix*zlev(ig,l))<0.) THEN PRINT *, 'pb l_mix*zlev<0' END IF ! CR: test: nouvelle def de lambda ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) IF (zw2(ig,l)>1.E-10) THEN larg_detr(ig, l) = sqrt((l_mix/zw2(ig,l))*zlev(ig,l)) ELSE larg_detr(ig, l) = sqrt(l_mix*zlev(ig,l)) END IF ! else if (idetr.eq.1) then ! larg_detr(ig,l)=larg_cons(ig,l) ! s *sqrt(l_mix*zlev(ig,l))/larg_cons(ig,lmix(ig)) ! else if (idetr.eq.2) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *sqrt(wa_moy(ig,l)) ! else if (idetr.eq.4) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *wa_moy(ig,l) ! endif END IF END DO END DO ! print*,'10 OK convect8' ! print*,'WA2 ',wa_moy ! cal1cul de la fraction de la maille concernée par l'ascendance en tenant ! compte de l'epluchage du thermique. DO l = 2, nlay DO ig = 1, ngrid IF (larg_cons(ig,l)>1. .AND. (test(ig)==1)) THEN ! print*,ig,l,lmix(ig),lmaxa(ig),larg_cons(ig,l),' KKK' fraca(ig, l) = (larg_cons(ig,l)-larg_detr(ig,l))/(r_aspect*zmax(ig)) ! test fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) ELSE ! wa_moy(ig,l)=0. fraca(ig, l) = 0. fracc(ig, l) = 0. fracd(ig, l) = 1. END IF END DO END DO ! CR: calcul de fracazmix DO ig = 1, ngrid IF (test(ig)==1) THEN fracazmix(ig) = (fraca(ig,lmix(ig)+1)-fraca(ig,lmix(ig)))/ & (zlev(ig,lmix(ig)+1)-zlev(ig,lmix(ig)))*zmix(ig) + & fraca(ig, lmix(ig)) - zlev(ig, lmix(ig))*(fraca(ig,lmix(ig)+1)-fraca( & ig,lmix(ig)))/(zlev(ig,lmix(ig)+1)-zlev(ig,lmix(ig))) END IF END DO DO l = 2, nlay DO ig = 1, ngrid IF (larg_cons(ig,l)>1. .AND. (test(ig)==1)) THEN IF (l>lmix(ig)) THEN ! test IF (zmax(ig)-zmix(ig)<1.E-10) THEN ! print*,'pb xxx' xxx(ig, l) = (lmax(ig)+1.-l)/(lmax(ig)+1.-lmix(ig)) ELSE xxx(ig, l) = (zmax(ig)-zlev(ig,l))/(zmax(ig)-zmix(ig)) END IF IF (idetr==0) THEN fraca(ig, l) = fracazmix(ig) ELSE IF (idetr==1) THEN fraca(ig, l) = fracazmix(ig)*xxx(ig, l) ELSE IF (idetr==2) THEN fraca(ig, l) = fracazmix(ig)*(1.-(1.-xxx(ig,l))**2) ELSE fraca(ig, l) = fracazmix(ig)*xxx(ig, l)**2 END IF ! print*,ig,l,lmix(ig),lmaxa(ig),xxx(ig,l),'LLLLLLL' fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) END IF END IF END DO END DO PRINT *, 'fin calcul fraca' ! print*,'11 OK convect8' ! print*,'Ea3 ',wa_moy ! ------------------------------------------------------------------ ! Calcul de fracd, wd ! somme wa - wd = 0 ! ------------------------------------------------------------------ DO ig = 1, ngrid fm(ig, 1) = 0. fm(ig, nlay+1) = 0. END DO DO l = 2, nlay DO ig = 1, ngrid IF (test(ig)==1) THEN fm(ig, l) = fraca(ig, l)*wa_moy(ig, l)*rhobarz(ig, l) ! CR:test IF (alim(ig,l-1)<1E-10 .AND. fm(ig,l)>fm(ig,l-1) .AND. l>lmix(ig)) & THEN fm(ig, l) = fm(ig, l-1) ! write(1,*)'ajustement fm, l',l END IF ! write(1,*)'ig,l,fm(ig,l)',ig,l,fm(ig,l) ! RC END IF END DO DO ig = 1, ngrid IF (fracd(ig,l)<0.1 .AND. (test(ig)==1)) THEN abort_message = 'fracd trop petit' CALL abort_physic(modname, abort_message, 1) ELSE ! vitesse descendante "diagnostique" wd(ig, l) = fm(ig, l)/(fracd(ig,l)*rhobarz(ig,l)) END IF END DO END DO DO l = 1, nlay + 1 DO ig = 1, ngrid IF (test(ig)==0) THEN fm(ig, l) = fmc(ig, l) END IF END DO END DO ! fin du first DO l = 1, nlay DO ig = 1, ngrid ! masse(ig,l)=rho(ig,l)*(zlev(ig,l+1)-zlev(ig,l)) masse(ig, l) = (pplev(ig,l)-pplev(ig,l+1))/rg END DO END DO ! print*,'12 OK convect8' ! print*,'WA4 ',wa_moy ! c------------------------------------------------------------------ ! calcul du transport vertical ! ------------------------------------------------------------------ GO TO 4444 ! print*,'XXXXXXXXXXXXXXX ptimestep= ',ptimestep DO l = 2, nlay - 1 DO ig = 1, ngrid IF (fm(ig,l+1)*ptimestep>masse(ig,l) .AND. fm(ig,l+1)*ptimestep>masse( & ig,l+1)) THEN PRINT *, 'WARN!!! FM>M ig=', ig, ' l=', l, ' FM=', & fm(ig, l+1)*ptimestep, ' M=', masse(ig, l), masse(ig, l+1) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF ((alim(ig,l)+entr(ig,l))*ptimestep>masse(ig,l)) THEN PRINT *, 'WARN!!! E>M ig=', ig, ' l=', l, ' E==', & (entr(ig,l)+alim(ig,l))*ptimestep, ' M=', masse(ig, l) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (.NOT. fm(ig,l)>=0. .OR. .NOT. fm(ig,l)<=10.) THEN ! print*,'WARN!!! fm exagere ig=',ig,' l=',l ! s ,' FM=',fm(ig,l) END IF IF (.NOT. masse(ig,l)>=1.E-10 .OR. .NOT. masse(ig,l)<=1.E4) THEN ! print*,'WARN!!! masse exagere ig=',ig,' l=',l ! s ,' M=',masse(ig,l) ! print*,'rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l)', ! s rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l) ! print*,'zlev(ig,l+1),zlev(ig,l)' ! s ,zlev(ig,l+1),zlev(ig,l) ! print*,'pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1)' ! s ,pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1) END IF IF (.NOT. alim(ig,l)>=0. .OR. .NOT. alim(ig,l)<=10.) THEN ! print*,'WARN!!! entr exagere ig=',ig,' l=',l ! s ,' E=',entr(ig,l) END IF END DO END DO 4444 CONTINUE ! CR:redefinition du entr ! CR:test:on ne change pas la def du entr mais la def du fm DO l = 1, nlay DO ig = 1, ngrid IF (test(ig)==1) THEN detr(ig, l) = fm(ig, l) + alim(ig, l) - fm(ig, l+1) IF (detr(ig,l)<0.) THEN ! entr(ig,l)=entr(ig,l)-detr(ig,l) fm(ig, l+1) = fm(ig, l) + alim(ig, l) detr(ig, l) = 0. ! write(11,*)'l,ig,entr',l,ig,entr(ig,l) ! print*,'WARNING !!! detrainement negatif ',ig,l END IF END IF END DO END DO ! RC IF (w2di==1) THEN fm0 = fm0 + ptimestep*(fm-fm0)/tho entr0 = entr0 + ptimestep*(alim+entr-entr0)/tho ELSE fm0 = fm entr0 = alim + entr detr0 = detr alim0 = alim ! zoa=zqta ! entr0=alim END IF IF (1==1) THEN ! call dqthermcell(ngrid,nlay,ptimestep,fm0,entr0,masse ! . ,zh,zdhadj,zha) ! call dqthermcell(ngrid,nlay,ptimestep,fm0,entr0,masse ! . ,zo,pdoadj,zoa) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zthl, & zdthladj, zta) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, po, pdoadj, & zoa) ELSE CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zh, & zdhadj, zha) CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zo, & pdoadj, zoa) END IF IF (1==0) THEN CALL dvthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zmax, & zu, zv, pduadj, pdvadj, zua, zva) ELSE CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zu, pduadj, & zua) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zv, pdvadj, & zva) END IF ! Calcul des moments ! do l=1,nlay ! do ig=1,ngrid ! zf=0.5*(fracc(ig,l)+fracc(ig,l+1)) ! zf2=zf/(1.-zf) ! thetath2(ig,l)=zf2*(zha(ig,l)-zh(ig,l))**2 ! wth2(ig,l)=zf2*(0.5*(wa_moy(ig,l)+wa_moy(ig,l+1)))**2 ! enddo ! enddo ! print*,'13 OK convect8' ! print*,'WA5 ',wa_moy DO l = 1, nlay DO ig = 1, ngrid ! pdtadj(ig,l)=zdhadj(ig,l)*zpspsk(ig,l) pdtadj(ig, l) = zdthladj(ig, l)*zpspsk(ig, l) END DO END DO ! do l=1,nlay ! do ig=1,ngrid ! if(abs(pdtadj(ig,l))*86400..gt.500.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdtadj=',pdtadj(ig,l) ! endif ! if(abs(pdoadj(ig,l))*86400..gt.1.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdoadj=',pdoadj(ig,l) ! endif ! enddo ! enddo ! print*,'14 OK convect8' ! ------------------------------------------------------------------ ! Calculs pour les sorties ! ------------------------------------------------------------------ ! calcul de fraca pour les sorties DO l = 2, klev DO ig = 1, klon IF (zw2(ig,l)>1.E-10) THEN fraca(ig, l) = fm(ig, l)/(rhobarz(ig,l)*zw2(ig,l)) ELSE fraca(ig, l) = 0. END IF END DO END DO IF (sorties) THEN DO l = 1, nlay DO ig = 1, ngrid zla(ig, l) = (1.-fracd(ig,l))*zmax(ig) zld(ig, l) = fracd(ig, l)*zmax(ig) IF (1.-fracd(ig,l)>1.E-10) zwa(ig, l) = wd(ig, l)*fracd(ig, l)/ & (1.-fracd(ig,l)) END DO END DO ! CR calcul du niveau de condensation ! initialisation DO ig = 1, ngrid nivcon(ig) = 0. zcon(ig) = 0. END DO DO k = nlay, 1, -1 DO ig = 1, ngrid IF (zqla(ig,k)>1E-10) THEN nivcon(ig) = k zcon(ig) = zlev(ig, k) END IF ! if (zcon(ig).gt.1.e-10) then ! nuage=.true. ! else ! nuage=.false. ! endif END DO END DO DO l = 1, nlay DO ig = 1, ngrid zf = fraca(ig, l) zf2 = zf/(1.-zf) thetath2(ig, l) = zf2*(zha(ig,l)-zh(ig,l)/zpspsk(ig,l))**2 wth2(ig, l) = zf2*(zw2(ig,l))**2 ! print*,'wth2=',wth2(ig,l) wth3(ig, l) = zf2*(1-2.*fraca(ig,l))/(1-fraca(ig,l))*zw2(ig, l)* & zw2(ig, l)*zw2(ig, l) q2(ig, l) = zf2*(zqta(ig,l)*1000.-po(ig,l)*1000.)**2 ! test: on calcul q2/po=ratqsc ! if (nuage) then ratqscth(ig, l) = sqrt(q2(ig,l))/(po(ig,l)*1000.) ! else ! ratqscth(ig,l)=0. ! endif END DO END DO ! calcul du ratqscdiff sum = 0. sumdiff = 0. ratqsdiff(:, :) = 0. DO ig = 1, ngrid DO l = 1, lentr(ig) sum = sum + alim_star(ig, l)*zqta(ig, l)*1000. END DO END DO DO ig = 1, ngrid DO l = 1, lentr(ig) zf = fraca(ig, l) zf2 = zf/(1.-zf) sumdiff = sumdiff + alim_star(ig, l)*(zqta(ig,l)*1000.-sum)**2 ! ratqsdiff=ratqsdiff+alim_star(ig,l)* ! s (zqta(ig,l)*1000.-po(ig,l)*1000.)**2 END DO END DO DO l = 1, klev DO ig = 1, ngrid ratqsdiff(ig, l) = sqrt(sumdiff)/(po(ig,l)*1000.) ! write(11,*)'ratqsdiff=',ratqsdiff(ig,l) END DO END DO END IF ! print*,'19 OK convect8' RETURN END SUBROUTINE thermcell_cld SUBROUTINE thermcell_eau(ngrid, nlay, ptimestep, pplay, pplev, pphi, pu, pv, & pt, po, pduadj, pdvadj, pdtadj, pdoadj, fm0, entr0 & ! s ! ,pu_therm,pv_therm , r_aspect, l_mix, w2di, tho) USE dimphy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! Réécriture à partir d'un listing papier à Habas, le 14/02/00 ! le thermique est supposé homogène et dissipé par mélange avec ! son environnement. la longueur l_mix contrôle l'efficacité du ! mélange ! Le calcul du transport des différentes espèces se fait en prenant ! en compte: ! 1. un flux de masse montant ! 2. un flux de masse descendant ! 3. un entrainement ! 4. un detrainement ! ======================================================================= ! ----------------------------------------------------------------------- ! declarations: ! ------------- include "dimensions.h" ! ccc#include "dimphy.h" include "YOMCST.h" include "YOETHF.h" include "FCTTRE.h" ! arguments: ! ---------- INTEGER ngrid, nlay, w2di REAL tho REAL ptimestep, l_mix, r_aspect REAL pt(ngrid, nlay), pdtadj(ngrid, nlay) REAL pu(ngrid, nlay), pduadj(ngrid, nlay) REAL pv(ngrid, nlay), pdvadj(ngrid, nlay) REAL po(ngrid, nlay), pdoadj(ngrid, nlay) REAL pplay(ngrid, nlay), pplev(ngrid, nlay+1) REAL pphi(ngrid, nlay) INTEGER idetr SAVE idetr DATA idetr/3/ !$OMP THREADPRIVATE(idetr) ! local: ! ------ INTEGER ig, k, l, lmaxa(klon), lmix(klon) REAL zsortie1d(klon) ! CR: on remplace lmax(klon,klev+1) INTEGER lmax(klon), lmin(klon), lentr(klon) REAL linter(klon) REAL zmix(klon), fracazmix(klon) ! RC REAL zmax(klon), zw, zz, zw2(klon, klev+1), ztva(klon, klev), zzz REAL zlev(klon, klev+1), zlay(klon, klev) REAL zh(klon, klev), zdhadj(klon, klev) REAL zthl(klon, klev), zdthladj(klon, klev) REAL ztv(klon, klev) REAL zu(klon, klev), zv(klon, klev), zo(klon, klev) REAL zl(klon, klev) REAL wh(klon, klev+1) REAL wu(klon, klev+1), wv(klon, klev+1), wo(klon, klev+1) REAL zla(klon, klev+1) REAL zwa(klon, klev+1) REAL zld(klon, klev+1) REAL zwd(klon, klev+1) REAL zsortie(klon, klev) REAL zva(klon, klev) REAL zua(klon, klev) REAL zoa(klon, klev) REAL zta(klon, klev) REAL zha(klon, klev) REAL wa_moy(klon, klev+1) REAL fraca(klon, klev+1) REAL fracc(klon, klev+1) REAL zf, zf2 REAL thetath2(klon, klev), wth2(klon, klev) ! common/comtherm/thetath2,wth2 REAL count_time INTEGER ialt LOGICAL sorties REAL rho(klon, klev), rhobarz(klon, klev+1), masse(klon, klev) REAL zpspsk(klon, klev) ! real wmax(klon,klev),wmaxa(klon) REAL wmax(klon), wmaxa(klon) REAL wa(klon, klev, klev+1) REAL wd(klon, klev+1) REAL larg_part(klon, klev, klev+1) REAL fracd(klon, klev+1) REAL xxx(klon, klev+1) REAL larg_cons(klon, klev+1) REAL larg_detr(klon, klev+1) REAL fm0(klon, klev+1), entr0(klon, klev), detr(klon, klev) REAL pu_therm(klon, klev), pv_therm(klon, klev) REAL fm(klon, klev+1), entr(klon, klev) REAL fmc(klon, klev+1) REAL zcor, zdelta, zcvm5, qlbef REAL tbef(klon), qsatbef(klon) REAL dqsat_dt, dt, num, denom REAL reps, rlvcp, ddt0 REAL ztla(klon, klev), zqla(klon, klev), zqta(klon, klev) PARAMETER (ddt0=.01) ! CR:nouvelles variables REAL f_star(klon, klev+1), entr_star(klon, klev) REAL entr_star_tot(klon), entr_star2(klon) REAL f(klon), f0(klon) REAL zlevinter(klon) LOGICAL first DATA first/.FALSE./ SAVE first !$OMP THREADPRIVATE(first) ! RC CHARACTER *2 str2 CHARACTER *10 str10 CHARACTER (LEN=20) :: modname = 'thermcell_eau' CHARACTER (LEN=80) :: abort_message LOGICAL vtest(klon), down LOGICAL zsat(klon) EXTERNAL scopy INTEGER ncorrec, ll SAVE ncorrec DATA ncorrec/0/ !$OMP THREADPRIVATE(ncorrec) ! ----------------------------------------------------------------------- ! initialisation: ! --------------- sorties = .TRUE. IF (ngrid/=klon) THEN PRINT * PRINT *, 'STOP dans convadj' PRINT *, 'ngrid =', ngrid PRINT *, 'klon =', klon END IF ! Initialisation rlvcp = rlvtt/rcpd reps = rd/rv ! ----------------------------------------------------------------------- ! AM Calcul de T,q,ql a partir de Tl et qT ! --------------------------------------------------- ! Pr Tprec=Tl calcul de qsat ! Si qsat>qT T=Tl, q=qT ! Sinon DDT=(-Tprec+Tl+RLVCP (qT-qsat(T')) / (1+RLVCP dqsat/dt) ! On cherche DDT < DDT0 ! defaut DO ll = 1, nlay DO ig = 1, ngrid zo(ig, ll) = po(ig, ll) zl(ig, ll) = 0. zh(ig, ll) = pt(ig, ll) END DO END DO DO ig = 1, ngrid zsat(ig) = .FALSE. END DO DO ll = 1, nlay ! les points insatures sont definitifs DO ig = 1, ngrid tbef(ig) = pt(ig, ll) zdelta = max(0., sign(1.,rtt-tbef(ig))) qsatbef(ig) = r2es*foeew(tbef(ig), zdelta)/pplev(ig, ll) qsatbef(ig) = min(0.5, qsatbef(ig)) zcor = 1./(1.-retv*qsatbef(ig)) qsatbef(ig) = qsatbef(ig)*zcor zsat(ig) = (max(0.,po(ig,ll)-qsatbef(ig))>0.00001) END DO DO ig = 1, ngrid IF (zsat(ig)) THEN qlbef = max(0., po(ig,ll)-qsatbef(ig)) ! si sature: ql est surestime, d'ou la sous-relax dt = 0.5*rlvcp*qlbef ! on pourra enchainer 2 ou 3 calculs sans Do while DO WHILE (dt>ddt0) ! il faut verifier si c,a conserve quand on repasse en insature ... tbef(ig) = tbef(ig) + dt zdelta = max(0., sign(1.,rtt-tbef(ig))) qsatbef(ig) = r2es*foeew(tbef(ig), zdelta)/pplev(ig, ll) qsatbef(ig) = min(0.5, qsatbef(ig)) zcor = 1./(1.-retv*qsatbef(ig)) qsatbef(ig) = qsatbef(ig)*zcor ! on veut le signe de qlbef qlbef = po(ig, ll) - qsatbef(ig) ! dqsat_dT zdelta = max(0., sign(1.,rtt-tbef(ig))) zcvm5 = r5les*(1.-zdelta) + r5ies*zdelta zcor = 1./(1.-retv*qsatbef(ig)) dqsat_dt = foede(tbef(ig), zdelta, zcvm5, qsatbef(ig), zcor) num = -tbef(ig) + pt(ig, ll) + rlvcp*qlbef denom = 1. + rlvcp*dqsat_dt dt = num/denom END DO ! on ecrit de maniere conservative (sat ou non) zl(ig, ll) = max(0., qlbef) ! T = Tl +Lv/Cp ql zh(ig, ll) = pt(ig, ll) + rlvcp*zl(ig, ll) zo(ig, ll) = po(ig, ll) - zl(ig, ll) END IF END DO END DO ! AM fin ! ----------------------------------------------------------------------- ! incrementation eventuelle de tendances precedentes: ! --------------------------------------------------- ! print*,'0 OK convect8' DO l = 1, nlay DO ig = 1, ngrid zpspsk(ig, l) = (pplay(ig,l)/pplev(ig,1))**rkappa ! zh(ig,l)=pt(ig,l)/zpspsk(ig,l) zu(ig, l) = pu(ig, l) zv(ig, l) = pv(ig, l) ! zo(ig,l)=po(ig,l) ! ztv(ig,l)=zh(ig,l)*(1.+0.61*zo(ig,l)) ! AM attention zh est maintenant le profil de T et plus le profil de ! theta ! ! T-> Theta ztv(ig, l) = zh(ig, l)/zpspsk(ig, l) ! AM Theta_v ztv(ig, l) = ztv(ig, l)*(1.+retv*(zo(ig,l))-zl(ig,l)) ! AM Thetal zthl(ig, l) = pt(ig, l)/zpspsk(ig, l) END DO END DO ! print*,'1 OK convect8' ! -------------------- ! + + + + + + + + + + + ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz ! wh,wt,wo ... ! + + + + + + + + + + + zh,zu,zv,zo,rho ! -------------------- zlev(1) ! \\\\\\\\\\\\\\\\\\\\ ! ----------------------------------------------------------------------- ! Calcul des altitudes des couches ! ----------------------------------------------------------------------- DO l = 2, nlay DO ig = 1, ngrid zlev(ig, l) = 0.5*(pphi(ig,l)+pphi(ig,l-1))/rg END DO END DO DO ig = 1, ngrid zlev(ig, 1) = 0. zlev(ig, nlay+1) = (2.*pphi(ig,klev)-pphi(ig,klev-1))/rg END DO DO l = 1, nlay DO ig = 1, ngrid zlay(ig, l) = pphi(ig, l)/rg END DO END DO ! print*,'2 OK convect8' ! ----------------------------------------------------------------------- ! Calcul des densites ! ----------------------------------------------------------------------- DO l = 1, nlay DO ig = 1, ngrid ! rho(ig,l)=pplay(ig,l)/(zpspsk(ig,l)*RD*zh(ig,l)) rho(ig, l) = pplay(ig, l)/(zpspsk(ig,l)*rd*ztv(ig,l)) END DO END DO DO l = 2, nlay DO ig = 1, ngrid rhobarz(ig, l) = 0.5*(rho(ig,l)+rho(ig,l-1)) END DO END DO DO k = 1, nlay DO l = 1, nlay + 1 DO ig = 1, ngrid wa(ig, k, l) = 0. END DO END DO END DO ! print*,'3 OK convect8' ! ------------------------------------------------------------------ ! Calcul de w2, quarre de w a partir de la cape ! a partir de w2, on calcule wa, vitesse de l'ascendance ! ATTENTION: Dans cette version, pour cause d'economie de memoire, ! w2 est stoke dans wa ! ATTENTION: dans convect8, on n'utilise le calcule des wa ! independants par couches que pour calculer l'entrainement ! a la base et la hauteur max de l'ascendance. ! Indicages: ! l'ascendance provenant du niveau k traverse l'interface l avec ! une vitesse wa(k,l). ! -------------------- ! + + + + + + + + + + ! wa(k,l) ---- -------------------- l ! /\ ! /||\ + + + + + + + + + + ! || ! || -------------------- ! || ! || + + + + + + + + + + ! || ! || -------------------- ! ||__ ! |___ + + + + + + + + + + k ! -------------------- ! ------------------------------------------------------------------ ! CR: ponderation entrainement des couches instables ! def des entr_star tels que entr=f*entr_star DO l = 1, klev DO ig = 1, ngrid entr_star(ig, l) = 0. END DO END DO ! determination de la longueur de la couche d entrainement DO ig = 1, ngrid lentr(ig) = 1 END DO ! on ne considere que les premieres couches instables DO k = nlay - 1, 1, -1 DO ig = 1, ngrid IF (ztv(ig,k)>ztv(ig,k+1) .AND. ztv(ig,k+1)ztv(ig,l)) THEN lmin(ig) = l - 1 END IF END DO END DO ! definition de l'entrainement des couches DO l = 1, klev - 1 DO ig = 1, ngrid IF (ztv(ig,l)>ztv(ig,l+1) .AND. l>=lmin(ig) .AND. l<=lentr(ig)) THEN entr_star(ig, l) = (ztv(ig,l)-ztv(ig,l+1))*(zlev(ig,l+1)-zlev(ig,l)) END IF END DO END DO ! pas de thermique si couche 1 stable DO ig = 1, ngrid IF (lmin(ig)>1) THEN DO l = 1, klev entr_star(ig, l) = 0. END DO END IF END DO ! calcul de l entrainement total DO ig = 1, ngrid entr_star_tot(ig) = 0. END DO DO ig = 1, ngrid DO k = 1, klev entr_star_tot(ig) = entr_star_tot(ig) + entr_star(ig, k) END DO END DO DO k = 1, klev DO ig = 1, ngrid ztva(ig, k) = ztv(ig, k) END DO END DO ! RC ! AM:initialisations DO k = 1, nlay DO ig = 1, ngrid ztva(ig, k) = ztv(ig, k) ztla(ig, k) = zthl(ig, k) zqla(ig, k) = 0. zqta(ig, k) = po(ig, k) zsat(ig) = .FALSE. END DO END DO ! print*,'7 OK convect8' DO k = 1, klev + 1 DO ig = 1, ngrid zw2(ig, k) = 0. fmc(ig, k) = 0. ! CR f_star(ig, k) = 0. ! RC larg_cons(ig, k) = 0. larg_detr(ig, k) = 0. wa_moy(ig, k) = 0. END DO END DO ! print*,'8 OK convect8' DO ig = 1, ngrid linter(ig) = 1. lmaxa(ig) = 1 lmix(ig) = 1 wmaxa(ig) = 0. END DO ! CR: DO l = 1, nlay - 2 DO ig = 1, ngrid IF (ztv(ig,l)>ztv(ig,l+1) .AND. entr_star(ig,l)>1.E-10 .AND. & zw2(ig,l)<1E-10) THEN ! AM ztla(ig, l) = zthl(ig, l) zqta(ig, l) = po(ig, l) zqla(ig, l) = zl(ig, l) ! AM f_star(ig, l+1) = entr_star(ig, l) ! test:calcul de dteta zw2(ig, l+1) = 2.*rg*(ztv(ig,l)-ztv(ig,l+1))/ztv(ig, l+1)* & (zlev(ig,l+1)-zlev(ig,l))*0.4*pphi(ig, l)/(pphi(ig,l+1)-pphi(ig,l)) larg_detr(ig, l) = 0. ELSE IF ((zw2(ig,l)>=1E-10) .AND. (f_star(ig,l)+entr_star(ig, & l)>1.E-10)) THEN f_star(ig, l+1) = f_star(ig, l) + entr_star(ig, l) ! AM on melange Tl et qt du thermique ztla(ig, l) = (f_star(ig,l)*ztla(ig,l-1)+entr_star(ig,l)*zthl(ig,l))/ & f_star(ig, l+1) zqta(ig, l) = (f_star(ig,l)*zqta(ig,l-1)+entr_star(ig,l)*po(ig,l))/ & f_star(ig, l+1) ! ztva(ig,l)=(f_star(ig,l)*ztva(ig,l-1)+entr_star(ig,l) ! s *ztv(ig,l))/f_star(ig,l+1) ! AM on en deduit thetav et ql du thermique tbef(ig) = ztla(ig, l)*zpspsk(ig, l) zdelta = max(0., sign(1.,rtt-tbef(ig))) qsatbef(ig) = r2es*foeew(tbef(ig), zdelta)/pplev(ig, l) qsatbef(ig) = min(0.5, qsatbef(ig)) zcor = 1./(1.-retv*qsatbef(ig)) qsatbef(ig) = qsatbef(ig)*zcor zsat(ig) = (max(0.,zqta(ig,l)-qsatbef(ig))>0.00001) END IF END DO DO ig = 1, ngrid IF (zsat(ig)) THEN qlbef = max(0., zqta(ig,l)-qsatbef(ig)) dt = 0.5*rlvcp*qlbef DO WHILE (dt>ddt0) tbef(ig) = tbef(ig) + dt zdelta = max(0., sign(1.,rtt-tbef(ig))) qsatbef(ig) = r2es*foeew(tbef(ig), zdelta)/pplev(ig, l) qsatbef(ig) = min(0.5, qsatbef(ig)) zcor = 1./(1.-retv*qsatbef(ig)) qsatbef(ig) = qsatbef(ig)*zcor qlbef = zqta(ig, l) - qsatbef(ig) zdelta = max(0., sign(1.,rtt-tbef(ig))) zcvm5 = r5les*(1.-zdelta) + r5ies*zdelta zcor = 1./(1.-retv*qsatbef(ig)) dqsat_dt = foede(tbef(ig), zdelta, zcvm5, qsatbef(ig), zcor) num = -tbef(ig) + ztla(ig, l)*zpspsk(ig, l) + rlvcp*qlbef denom = 1. + rlvcp*dqsat_dt dt = num/denom END DO zqla(ig, l) = max(0., zqta(ig,l)-qsatbef(ig)) END IF ! on ecrit de maniere conservative (sat ou non) ! T = Tl +Lv/Cp ql ztva(ig, l) = ztla(ig, l)*zpspsk(ig, l) + rlvcp*zqla(ig, l) ztva(ig, l) = ztva(ig, l)/zpspsk(ig, l) ztva(ig, l) = ztva(ig, l)*(1.+retv*(zqta(ig,l)-zqla(ig,l))-zqla(ig,l)) END DO DO ig = 1, ngrid IF (zw2(ig,l)>=1.E-10 .AND. f_star(ig,l)+entr_star(ig,l)>1.E-10) THEN ! mise a jour de la vitesse ascendante (l'air entraine de la couche ! consideree commence avec une vitesse nulle). zw2(ig, l+1) = zw2(ig, l)*(f_star(ig,l)/f_star(ig,l+1))**2 + & 2.*rg*(ztva(ig,l)-ztv(ig,l))/ztv(ig, l)*(zlev(ig,l+1)-zlev(ig,l)) END IF ! determination de zmax continu par interpolation lineaire IF (zw2(ig,l+1)<0.) THEN linter(ig) = (l*(zw2(ig,l+1)-zw2(ig,l))-zw2(ig,l))/(zw2(ig,l+1)-zw2( & ig,l)) zw2(ig, l+1) = 0. lmaxa(ig) = l ELSE wa_moy(ig, l+1) = sqrt(zw2(ig,l+1)) END IF IF (wa_moy(ig,l+1)>wmaxa(ig)) THEN ! lmix est le niveau de la couche ou w (wa_moy) est maximum lmix(ig) = l + 1 wmaxa(ig) = wa_moy(ig, l+1) END IF END DO END DO ! Calcul de la couche correspondant a la hauteur du thermique DO ig = 1, ngrid lmax(ig) = lentr(ig) END DO DO ig = 1, ngrid DO l = nlay, lentr(ig) + 1, -1 IF (zw2(ig,l)<=1.E-10) THEN lmax(ig) = l - 1 END IF END DO END DO ! pas de thermique si couche 1 stable DO ig = 1, ngrid IF (lmin(ig)>1) THEN lmax(ig) = 1 lmin(ig) = 1 END IF END DO ! Determination de zw2 max DO ig = 1, ngrid wmax(ig) = 0. END DO DO l = 1, nlay DO ig = 1, ngrid IF (l<=lmax(ig)) THEN zw2(ig, l) = sqrt(zw2(ig,l)) wmax(ig) = max(wmax(ig), zw2(ig,l)) ELSE zw2(ig, l) = 0. END IF END DO END DO ! Longueur caracteristique correspondant a la hauteur des thermiques. DO ig = 1, ngrid zmax(ig) = 500. zlevinter(ig) = zlev(ig, 1) END DO DO ig = 1, ngrid ! calcul de zlevinter zlevinter(ig) = (zlev(ig,lmax(ig)+1)-zlev(ig,lmax(ig)))*linter(ig) + & zlev(ig, lmax(ig)) - lmax(ig)*(zlev(ig,lmax(ig)+1)-zlev(ig,lmax(ig))) zmax(ig) = max(zmax(ig), zlevinter(ig)-zlev(ig,lmin(ig))) END DO ! Fermeture,determination de f DO ig = 1, ngrid entr_star2(ig) = 0. END DO DO ig = 1, ngrid IF (entr_star_tot(ig)<1.E-10) THEN f(ig) = 0. ELSE DO k = lmin(ig), lentr(ig) entr_star2(ig) = entr_star2(ig) + entr_star(ig, k)**2/(rho(ig,k)*( & zlev(ig,k+1)-zlev(ig,k))) END DO ! Nouvelle fermeture f(ig) = wmax(ig)/(zmax(ig)*r_aspect*entr_star2(ig))*entr_star_tot(ig) ! test IF (first) THEN f(ig) = f(ig) + (f0(ig)-f(ig))*exp(-ptimestep/zmax(ig)*wmax(ig)) END IF END IF f0(ig) = f(ig) first = .TRUE. END DO ! Calcul de l'entrainement DO k = 1, klev DO ig = 1, ngrid entr(ig, k) = f(ig)*entr_star(ig, k) END DO END DO ! Calcul des flux DO ig = 1, ngrid DO l = 1, lmax(ig) - 1 fmc(ig, l+1) = fmc(ig, l) + entr(ig, l) END DO END DO ! RC ! print*,'9 OK convect8' ! print*,'WA1 ',wa_moy ! determination de l'indice du debut de la mixed layer ou w decroit ! calcul de la largeur de chaque ascendance dans le cas conservatif. ! dans ce cas simple, on suppose que la largeur de l'ascendance provenant ! d'une couche est égale à la hauteur de la couche alimentante. ! La vitesse maximale dans l'ascendance est aussi prise comme estimation ! de la vitesse d'entrainement horizontal dans la couche alimentante. DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmaxa(ig)) THEN zw = max(wa_moy(ig,l), 1.E-10) larg_cons(ig, l) = zmax(ig)*r_aspect*fmc(ig, l)/(rhobarz(ig,l)*zw) END IF END DO END DO DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmaxa(ig)) THEN ! if (idetr.eq.0) then ! cette option est finalement en dur. larg_detr(ig, l) = sqrt(l_mix*zlev(ig,l)) ! else if (idetr.eq.1) then ! larg_detr(ig,l)=larg_cons(ig,l) ! s *sqrt(l_mix*zlev(ig,l))/larg_cons(ig,lmix(ig)) ! else if (idetr.eq.2) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *sqrt(wa_moy(ig,l)) ! else if (idetr.eq.4) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *wa_moy(ig,l) ! endif END IF END DO END DO ! print*,'10 OK convect8' ! print*,'WA2 ',wa_moy ! calcul de la fraction de la maille concernée par l'ascendance en tenant ! compte de l'epluchage du thermique. ! CR def de zmix continu (profil parabolique des vitesses) DO ig = 1, ngrid IF (lmix(ig)>1.) THEN zmix(ig) = ((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig))) & **2-(zlev(ig,lmix(ig)+1))**2)-(zw2(ig,lmix(ig))-zw2(ig, & lmix(ig)+1))*((zlev(ig,lmix(ig)-1))**2-(zlev(ig,lmix(ig)))**2))/ & (2.*((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)))- & (zlev(ig,lmix(ig)+1)))-(zw2(ig,lmix(ig))-zw2(ig,lmix(ig)+1))*((zlev( & ig,lmix(ig)-1))-(zlev(ig,lmix(ig)))))) ELSE zmix(ig) = 0. END IF END DO ! calcul du nouveau lmix correspondant DO ig = 1, ngrid DO l = 1, klev IF (zmix(ig)>=zlev(ig,l) .AND. zmix(ig)1.) THEN ! print*,ig,l,lmix(ig),lmaxa(ig),larg_cons(ig,l),' KKK' fraca(ig, l) = (larg_cons(ig,l)-larg_detr(ig,l))/(r_aspect*zmax(ig)) ! test fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) ELSE ! wa_moy(ig,l)=0. fraca(ig, l) = 0. fracc(ig, l) = 0. fracd(ig, l) = 1. END IF END DO END DO ! CR: calcul de fracazmix DO ig = 1, ngrid fracazmix(ig) = (fraca(ig,lmix(ig)+1)-fraca(ig,lmix(ig)))/ & (zlev(ig,lmix(ig)+1)-zlev(ig,lmix(ig)))*zmix(ig) + & fraca(ig, lmix(ig)) - zlev(ig, lmix(ig))*(fraca(ig,lmix(ig)+1)-fraca(ig & ,lmix(ig)))/(zlev(ig,lmix(ig)+1)-zlev(ig,lmix(ig))) END DO DO l = 2, nlay DO ig = 1, ngrid IF (larg_cons(ig,l)>1.) THEN IF (l>lmix(ig)) THEN xxx(ig, l) = (zmax(ig)-zlev(ig,l))/(zmax(ig)-zmix(ig)) IF (idetr==0) THEN fraca(ig, l) = fracazmix(ig) ELSE IF (idetr==1) THEN fraca(ig, l) = fracazmix(ig)*xxx(ig, l) ELSE IF (idetr==2) THEN fraca(ig, l) = fracazmix(ig)*(1.-(1.-xxx(ig,l))**2) ELSE fraca(ig, l) = fracazmix(ig)*xxx(ig, l)**2 END IF ! print*,ig,l,lmix(ig),lmaxa(ig),xxx(ig,l),'LLLLLLL' fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) END IF END IF END DO END DO ! print*,'11 OK convect8' ! print*,'Ea3 ',wa_moy ! ------------------------------------------------------------------ ! Calcul de fracd, wd ! somme wa - wd = 0 ! ------------------------------------------------------------------ DO ig = 1, ngrid fm(ig, 1) = 0. fm(ig, nlay+1) = 0. END DO DO l = 2, nlay DO ig = 1, ngrid fm(ig, l) = fraca(ig, l)*wa_moy(ig, l)*rhobarz(ig, l) ! CR:test IF (entr(ig,l-1)<1E-10 .AND. fm(ig,l)>fm(ig,l-1) .AND. l>lmix(ig)) THEN fm(ig, l) = fm(ig, l-1) ! write(1,*)'ajustement fm, l',l END IF ! write(1,*)'ig,l,fm(ig,l)',ig,l,fm(ig,l) ! RC END DO DO ig = 1, ngrid IF (fracd(ig,l)<0.1) THEN abort_message = 'fracd trop petit' CALL abort_physic(modname, abort_message, 1) ELSE ! vitesse descendante "diagnostique" wd(ig, l) = fm(ig, l)/(fracd(ig,l)*rhobarz(ig,l)) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid ! masse(ig,l)=rho(ig,l)*(zlev(ig,l+1)-zlev(ig,l)) masse(ig, l) = (pplev(ig,l)-pplev(ig,l+1))/rg END DO END DO ! print*,'12 OK convect8' ! print*,'WA4 ',wa_moy ! c------------------------------------------------------------------ ! calcul du transport vertical ! ------------------------------------------------------------------ GO TO 4444 ! print*,'XXXXXXXXXXXXXXX ptimestep= ',ptimestep DO l = 2, nlay - 1 DO ig = 1, ngrid IF (fm(ig,l+1)*ptimestep>masse(ig,l) .AND. fm(ig,l+1)*ptimestep>masse( & ig,l+1)) THEN ! print*,'WARN!!! FM>M ig=',ig,' l=',l,' FM=' ! s ,fm(ig,l+1)*ptimestep ! s ,' M=',masse(ig,l),masse(ig,l+1) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (entr(ig,l)*ptimestep>masse(ig,l)) THEN ! print*,'WARN!!! E>M ig=',ig,' l=',l,' E==' ! s ,entr(ig,l)*ptimestep ! s ,' M=',masse(ig,l) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (.NOT. fm(ig,l)>=0. .OR. .NOT. fm(ig,l)<=10.) THEN ! print*,'WARN!!! fm exagere ig=',ig,' l=',l ! s ,' FM=',fm(ig,l) END IF IF (.NOT. masse(ig,l)>=1.E-10 .OR. .NOT. masse(ig,l)<=1.E4) THEN ! print*,'WARN!!! masse exagere ig=',ig,' l=',l ! s ,' M=',masse(ig,l) ! print*,'rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l)', ! s rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l) ! print*,'zlev(ig,l+1),zlev(ig,l)' ! s ,zlev(ig,l+1),zlev(ig,l) ! print*,'pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1)' ! s ,pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1) END IF IF (.NOT. entr(ig,l)>=0. .OR. .NOT. entr(ig,l)<=10.) THEN ! print*,'WARN!!! entr exagere ig=',ig,' l=',l ! s ,' E=',entr(ig,l) END IF END DO END DO 4444 CONTINUE IF (w2di==1) THEN fm0 = fm0 + ptimestep*(fm-fm0)/tho entr0 = entr0 + ptimestep*(entr-entr0)/tho ELSE fm0 = fm entr0 = entr END IF IF (1==1) THEN ! call dqthermcell(ngrid,nlay,ptimestep,fm0,entr0,masse ! . ,zh,zdhadj,zha) ! call dqthermcell(ngrid,nlay,ptimestep,fm0,entr0,masse ! . ,zo,pdoadj,zoa) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zthl, & zdthladj, zta) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, po, pdoadj, & zoa) ELSE CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zh, & zdhadj, zha) CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zo, & pdoadj, zoa) END IF IF (1==0) THEN CALL dvthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zmax, & zu, zv, pduadj, pdvadj, zua, zva) ELSE CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zu, pduadj, & zua) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zv, pdvadj, & zva) END IF DO l = 1, nlay DO ig = 1, ngrid zf = 0.5*(fracc(ig,l)+fracc(ig,l+1)) zf2 = zf/(1.-zf) thetath2(ig, l) = zf2*(zha(ig,l)-zh(ig,l))**2 wth2(ig, l) = zf2*(0.5*(wa_moy(ig,l)+wa_moy(ig,l+1)))**2 END DO END DO ! print*,'13 OK convect8' ! print*,'WA5 ',wa_moy DO l = 1, nlay DO ig = 1, ngrid ! pdtadj(ig,l)=zdhadj(ig,l)*zpspsk(ig,l) pdtadj(ig, l) = zdthladj(ig, l)*zpspsk(ig, l) END DO END DO ! do l=1,nlay ! do ig=1,ngrid ! if(abs(pdtadj(ig,l))*86400..gt.500.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdtadj=',pdtadj(ig,l) ! endif ! if(abs(pdoadj(ig,l))*86400..gt.1.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdoadj=',pdoadj(ig,l) ! endif ! enddo ! enddo ! print*,'14 OK convect8' ! ------------------------------------------------------------------ ! Calculs pour les sorties ! ------------------------------------------------------------------ RETURN END SUBROUTINE thermcell_eau SUBROUTINE thermcell(ngrid, nlay, ptimestep, pplay, pplev, pphi, pu, pv, pt, & po, pduadj, pdvadj, pdtadj, pdoadj, fm0, entr0 & ! s ! ,pu_therm,pv_therm , r_aspect, l_mix, w2di, tho) USE dimphy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! Réécriture à partir d'un listing papier à Habas, le 14/02/00 ! le thermique est supposé homogène et dissipé par mélange avec ! son environnement. la longueur l_mix contrôle l'efficacité du ! mélange ! Le calcul du transport des différentes espèces se fait en prenant ! en compte: ! 1. un flux de masse montant ! 2. un flux de masse descendant ! 3. un entrainement ! 4. un detrainement ! ======================================================================= ! ----------------------------------------------------------------------- ! declarations: ! ------------- include "dimensions.h" ! ccc#include "dimphy.h" include "YOMCST.h" ! arguments: ! ---------- INTEGER ngrid, nlay, w2di REAL tho REAL ptimestep, l_mix, r_aspect REAL pt(ngrid, nlay), pdtadj(ngrid, nlay) REAL pu(ngrid, nlay), pduadj(ngrid, nlay) REAL pv(ngrid, nlay), pdvadj(ngrid, nlay) REAL po(ngrid, nlay), pdoadj(ngrid, nlay) REAL pplay(ngrid, nlay), pplev(ngrid, nlay+1) REAL pphi(ngrid, nlay) INTEGER idetr SAVE idetr DATA idetr/3/ !$OMP THREADPRIVATE(idetr) ! local: ! ------ INTEGER ig, k, l, lmaxa(klon), lmix(klon) REAL zsortie1d(klon) ! CR: on remplace lmax(klon,klev+1) INTEGER lmax(klon), lmin(klon), lentr(klon) REAL linter(klon) REAL zmix(klon), fracazmix(klon) ! RC REAL zmax(klon), zw, zz, zw2(klon, klev+1), ztva(klon, klev), zzz REAL zlev(klon, klev+1), zlay(klon, klev) REAL zh(klon, klev), zdhadj(klon, klev) REAL ztv(klon, klev) REAL zu(klon, klev), zv(klon, klev), zo(klon, klev) REAL wh(klon, klev+1) REAL wu(klon, klev+1), wv(klon, klev+1), wo(klon, klev+1) REAL zla(klon, klev+1) REAL zwa(klon, klev+1) REAL zld(klon, klev+1) REAL zwd(klon, klev+1) REAL zsortie(klon, klev) REAL zva(klon, klev) REAL zua(klon, klev) REAL zoa(klon, klev) REAL zha(klon, klev) REAL wa_moy(klon, klev+1) REAL fraca(klon, klev+1) REAL fracc(klon, klev+1) REAL zf, zf2 REAL thetath2(klon, klev), wth2(klon, klev) ! common/comtherm/thetath2,wth2 REAL count_time INTEGER ialt LOGICAL sorties REAL rho(klon, klev), rhobarz(klon, klev+1), masse(klon, klev) REAL zpspsk(klon, klev) ! real wmax(klon,klev),wmaxa(klon) REAL wmax(klon), wmaxa(klon) REAL wa(klon, klev, klev+1) REAL wd(klon, klev+1) REAL larg_part(klon, klev, klev+1) REAL fracd(klon, klev+1) REAL xxx(klon, klev+1) REAL larg_cons(klon, klev+1) REAL larg_detr(klon, klev+1) REAL fm0(klon, klev+1), entr0(klon, klev), detr(klon, klev) REAL pu_therm(klon, klev), pv_therm(klon, klev) REAL fm(klon, klev+1), entr(klon, klev) REAL fmc(klon, klev+1) ! CR:nouvelles variables REAL f_star(klon, klev+1), entr_star(klon, klev) REAL entr_star_tot(klon), entr_star2(klon) REAL f(klon), f0(klon) REAL zlevinter(klon) LOGICAL first DATA first/.FALSE./ SAVE first !$OMP THREADPRIVATE(first) ! RC CHARACTER *2 str2 CHARACTER *10 str10 CHARACTER (LEN=20) :: modname = 'thermcell' CHARACTER (LEN=80) :: abort_message LOGICAL vtest(klon), down EXTERNAL scopy INTEGER ncorrec, ll SAVE ncorrec DATA ncorrec/0/ !$OMP THREADPRIVATE(ncorrec) ! ----------------------------------------------------------------------- ! initialisation: ! --------------- sorties = .TRUE. IF (ngrid/=klon) THEN PRINT * PRINT *, 'STOP dans convadj' PRINT *, 'ngrid =', ngrid PRINT *, 'klon =', klon END IF ! ----------------------------------------------------------------------- ! incrementation eventuelle de tendances precedentes: ! --------------------------------------------------- ! print*,'0 OK convect8' DO l = 1, nlay DO ig = 1, ngrid zpspsk(ig, l) = (pplay(ig,l)/pplev(ig,1))**rkappa zh(ig, l) = pt(ig, l)/zpspsk(ig, l) zu(ig, l) = pu(ig, l) zv(ig, l) = pv(ig, l) zo(ig, l) = po(ig, l) ztv(ig, l) = zh(ig, l)*(1.+0.61*zo(ig,l)) END DO END DO ! print*,'1 OK convect8' ! -------------------- ! + + + + + + + + + + + ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz ! wh,wt,wo ... ! + + + + + + + + + + + zh,zu,zv,zo,rho ! -------------------- zlev(1) ! \\\\\\\\\\\\\\\\\\\\ ! ----------------------------------------------------------------------- ! Calcul des altitudes des couches ! ----------------------------------------------------------------------- DO l = 2, nlay DO ig = 1, ngrid zlev(ig, l) = 0.5*(pphi(ig,l)+pphi(ig,l-1))/rg END DO END DO DO ig = 1, ngrid zlev(ig, 1) = 0. zlev(ig, nlay+1) = (2.*pphi(ig,klev)-pphi(ig,klev-1))/rg END DO DO l = 1, nlay DO ig = 1, ngrid zlay(ig, l) = pphi(ig, l)/rg END DO END DO ! print*,'2 OK convect8' ! ----------------------------------------------------------------------- ! Calcul des densites ! ----------------------------------------------------------------------- DO l = 1, nlay DO ig = 1, ngrid rho(ig, l) = pplay(ig, l)/(zpspsk(ig,l)*rd*zh(ig,l)) END DO END DO DO l = 2, nlay DO ig = 1, ngrid rhobarz(ig, l) = 0.5*(rho(ig,l)+rho(ig,l-1)) END DO END DO DO k = 1, nlay DO l = 1, nlay + 1 DO ig = 1, ngrid wa(ig, k, l) = 0. END DO END DO END DO ! print*,'3 OK convect8' ! ------------------------------------------------------------------ ! Calcul de w2, quarre de w a partir de la cape ! a partir de w2, on calcule wa, vitesse de l'ascendance ! ATTENTION: Dans cette version, pour cause d'economie de memoire, ! w2 est stoke dans wa ! ATTENTION: dans convect8, on n'utilise le calcule des wa ! independants par couches que pour calculer l'entrainement ! a la base et la hauteur max de l'ascendance. ! Indicages: ! l'ascendance provenant du niveau k traverse l'interface l avec ! une vitesse wa(k,l). ! -------------------- ! + + + + + + + + + + ! wa(k,l) ---- -------------------- l ! /\ ! /||\ + + + + + + + + + + ! || ! || -------------------- ! || ! || + + + + + + + + + + ! || ! || -------------------- ! ||__ ! |___ + + + + + + + + + + k ! -------------------- ! ------------------------------------------------------------------ ! CR: ponderation entrainement des couches instables ! def des entr_star tels que entr=f*entr_star DO l = 1, klev DO ig = 1, ngrid entr_star(ig, l) = 0. END DO END DO ! determination de la longueur de la couche d entrainement DO ig = 1, ngrid lentr(ig) = 1 END DO ! on ne considere que les premieres couches instables DO k = nlay - 2, 1, -1 DO ig = 1, ngrid IF (ztv(ig,k)>ztv(ig,k+1) .AND. ztv(ig,k+1)<=ztv(ig,k+2)) THEN lentr(ig) = k END IF END DO END DO ! determination du lmin: couche d ou provient le thermique DO ig = 1, ngrid lmin(ig) = 1 END DO DO ig = 1, ngrid DO l = nlay, 2, -1 IF (ztv(ig,l-1)>ztv(ig,l)) THEN lmin(ig) = l - 1 END IF END DO END DO ! definition de l'entrainement des couches DO l = 1, klev - 1 DO ig = 1, ngrid IF (ztv(ig,l)>ztv(ig,l+1) .AND. l>=lmin(ig) .AND. l<=lentr(ig)) THEN entr_star(ig, l) = (ztv(ig,l)-ztv(ig,l+1))*(zlev(ig,l+1)-zlev(ig,l)) END IF END DO END DO ! pas de thermique si couches 1->5 stables DO ig = 1, ngrid IF (lmin(ig)>5) THEN DO l = 1, klev entr_star(ig, l) = 0. END DO END IF END DO ! calcul de l entrainement total DO ig = 1, ngrid entr_star_tot(ig) = 0. END DO DO ig = 1, ngrid DO k = 1, klev entr_star_tot(ig) = entr_star_tot(ig) + entr_star(ig, k) END DO END DO PRINT *, 'fin calcul entr_star' DO k = 1, klev DO ig = 1, ngrid ztva(ig, k) = ztv(ig, k) END DO END DO ! RC ! print*,'7 OK convect8' DO k = 1, klev + 1 DO ig = 1, ngrid zw2(ig, k) = 0. fmc(ig, k) = 0. ! CR f_star(ig, k) = 0. ! RC larg_cons(ig, k) = 0. larg_detr(ig, k) = 0. wa_moy(ig, k) = 0. END DO END DO ! print*,'8 OK convect8' DO ig = 1, ngrid linter(ig) = 1. lmaxa(ig) = 1 lmix(ig) = 1 wmaxa(ig) = 0. END DO ! CR: DO l = 1, nlay - 2 DO ig = 1, ngrid IF (ztv(ig,l)>ztv(ig,l+1) .AND. entr_star(ig,l)>1.E-10 .AND. & zw2(ig,l)<1E-10) THEN f_star(ig, l+1) = entr_star(ig, l) ! test:calcul de dteta zw2(ig, l+1) = 2.*rg*(ztv(ig,l)-ztv(ig,l+1))/ztv(ig, l+1)* & (zlev(ig,l+1)-zlev(ig,l))*0.4*pphi(ig, l)/(pphi(ig,l+1)-pphi(ig,l)) larg_detr(ig, l) = 0. ELSE IF ((zw2(ig,l)>=1E-10) .AND. (f_star(ig,l)+entr_star(ig, & l)>1.E-10)) THEN f_star(ig, l+1) = f_star(ig, l) + entr_star(ig, l) ztva(ig, l) = (f_star(ig,l)*ztva(ig,l-1)+entr_star(ig,l)*ztv(ig,l))/ & f_star(ig, l+1) zw2(ig, l+1) = zw2(ig, l)*(f_star(ig,l)/f_star(ig,l+1))**2 + & 2.*rg*(ztva(ig,l)-ztv(ig,l))/ztv(ig, l)*(zlev(ig,l+1)-zlev(ig,l)) END IF ! determination de zmax continu par interpolation lineaire IF (zw2(ig,l+1)<0.) THEN ! test IF (abs(zw2(ig,l+1)-zw2(ig,l))<1E-10) THEN PRINT *, 'pb linter' END IF linter(ig) = (l*(zw2(ig,l+1)-zw2(ig,l))-zw2(ig,l))/(zw2(ig,l+1)-zw2( & ig,l)) zw2(ig, l+1) = 0. lmaxa(ig) = l ELSE IF (zw2(ig,l+1)<0.) THEN PRINT *, 'pb1 zw2<0' END IF wa_moy(ig, l+1) = sqrt(zw2(ig,l+1)) END IF IF (wa_moy(ig,l+1)>wmaxa(ig)) THEN ! lmix est le niveau de la couche ou w (wa_moy) est maximum lmix(ig) = l + 1 wmaxa(ig) = wa_moy(ig, l+1) END IF END DO END DO PRINT *, 'fin calcul zw2' ! Calcul de la couche correspondant a la hauteur du thermique DO ig = 1, ngrid lmax(ig) = lentr(ig) END DO DO ig = 1, ngrid DO l = nlay, lentr(ig) + 1, -1 IF (zw2(ig,l)<=1.E-10) THEN lmax(ig) = l - 1 END IF END DO END DO ! pas de thermique si couches 1->5 stables DO ig = 1, ngrid IF (lmin(ig)>5) THEN lmax(ig) = 1 lmin(ig) = 1 END IF END DO ! Determination de zw2 max DO ig = 1, ngrid wmax(ig) = 0. END DO DO l = 1, nlay DO ig = 1, ngrid IF (l<=lmax(ig)) THEN IF (zw2(ig,l)<0.) THEN PRINT *, 'pb2 zw2<0' END IF zw2(ig, l) = sqrt(zw2(ig,l)) wmax(ig) = max(wmax(ig), zw2(ig,l)) ELSE zw2(ig, l) = 0. END IF END DO END DO ! Longueur caracteristique correspondant a la hauteur des thermiques. DO ig = 1, ngrid zmax(ig) = 0. zlevinter(ig) = zlev(ig, 1) END DO DO ig = 1, ngrid ! calcul de zlevinter zlevinter(ig) = (zlev(ig,lmax(ig)+1)-zlev(ig,lmax(ig)))*linter(ig) + & zlev(ig, lmax(ig)) - lmax(ig)*(zlev(ig,lmax(ig)+1)-zlev(ig,lmax(ig))) zmax(ig) = max(zmax(ig), zlevinter(ig)-zlev(ig,lmin(ig))) END DO PRINT *, 'avant fermeture' ! Fermeture,determination de f DO ig = 1, ngrid entr_star2(ig) = 0. END DO DO ig = 1, ngrid IF (entr_star_tot(ig)<1.E-10) THEN f(ig) = 0. ELSE DO k = lmin(ig), lentr(ig) entr_star2(ig) = entr_star2(ig) + entr_star(ig, k)**2/(rho(ig,k)*( & zlev(ig,k+1)-zlev(ig,k))) END DO ! Nouvelle fermeture f(ig) = wmax(ig)/(max(500.,zmax(ig))*r_aspect*entr_star2(ig))* & entr_star_tot(ig) ! test ! if (first) then ! f(ig)=f(ig)+(f0(ig)-f(ig))*exp(-ptimestep/zmax(ig) ! s *wmax(ig)) ! endif END IF ! f0(ig)=f(ig) ! first=.true. END DO PRINT *, 'apres fermeture' ! Calcul de l'entrainement DO k = 1, klev DO ig = 1, ngrid entr(ig, k) = f(ig)*entr_star(ig, k) END DO END DO ! Calcul des flux DO ig = 1, ngrid DO l = 1, lmax(ig) - 1 fmc(ig, l+1) = fmc(ig, l) + entr(ig, l) END DO END DO ! RC ! print*,'9 OK convect8' ! print*,'WA1 ',wa_moy ! determination de l'indice du debut de la mixed layer ou w decroit ! calcul de la largeur de chaque ascendance dans le cas conservatif. ! dans ce cas simple, on suppose que la largeur de l'ascendance provenant ! d'une couche est égale à la hauteur de la couche alimentante. ! La vitesse maximale dans l'ascendance est aussi prise comme estimation ! de la vitesse d'entrainement horizontal dans la couche alimentante. DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmaxa(ig)) THEN zw = max(wa_moy(ig,l), 1.E-10) larg_cons(ig, l) = zmax(ig)*r_aspect*fmc(ig, l)/(rhobarz(ig,l)*zw) END IF END DO END DO DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmaxa(ig)) THEN ! if (idetr.eq.0) then ! cette option est finalement en dur. IF ((l_mix*zlev(ig,l))<0.) THEN PRINT *, 'pb l_mix*zlev<0' END IF larg_detr(ig, l) = sqrt(l_mix*zlev(ig,l)) ! else if (idetr.eq.1) then ! larg_detr(ig,l)=larg_cons(ig,l) ! s *sqrt(l_mix*zlev(ig,l))/larg_cons(ig,lmix(ig)) ! else if (idetr.eq.2) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *sqrt(wa_moy(ig,l)) ! else if (idetr.eq.4) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *wa_moy(ig,l) ! endif END IF END DO END DO ! print*,'10 OK convect8' ! print*,'WA2 ',wa_moy ! calcul de la fraction de la maille concernée par l'ascendance en tenant ! compte de l'epluchage du thermique. ! CR def de zmix continu (profil parabolique des vitesses) DO ig = 1, ngrid IF (lmix(ig)>1.) THEN ! test IF (((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)))- & (zlev(ig,lmix(ig)+1)))-(zw2(ig,lmix(ig))- & zw2(ig,lmix(ig)+1))*((zlev(ig,lmix(ig)-1))- & (zlev(ig,lmix(ig)))))>1E-10) THEN zmix(ig) = ((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)) & )**2-(zlev(ig,lmix(ig)+1))**2)-(zw2(ig,lmix(ig))-zw2(ig, & lmix(ig)+1))*((zlev(ig,lmix(ig)-1))**2-(zlev(ig,lmix(ig)))**2))/ & (2.*((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)))- & (zlev(ig,lmix(ig)+1)))-(zw2(ig,lmix(ig))- & zw2(ig,lmix(ig)+1))*((zlev(ig,lmix(ig)-1))-(zlev(ig,lmix(ig)))))) ELSE zmix(ig) = zlev(ig, lmix(ig)) PRINT *, 'pb zmix' END IF ELSE zmix(ig) = 0. END IF ! test IF ((zmax(ig)-zmix(ig))<0.) THEN zmix(ig) = 0.99*zmax(ig) ! print*,'pb zmix>zmax' END IF END DO ! calcul du nouveau lmix correspondant DO ig = 1, ngrid DO l = 1, klev IF (zmix(ig)>=zlev(ig,l) .AND. zmix(ig)1.) THEN ! print*,ig,l,lmix(ig),lmaxa(ig),larg_cons(ig,l),' KKK' fraca(ig, l) = (larg_cons(ig,l)-larg_detr(ig,l))/(r_aspect*zmax(ig)) ! test fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) ELSE ! wa_moy(ig,l)=0. fraca(ig, l) = 0. fracc(ig, l) = 0. fracd(ig, l) = 1. END IF END DO END DO ! CR: calcul de fracazmix DO ig = 1, ngrid fracazmix(ig) = (fraca(ig,lmix(ig)+1)-fraca(ig,lmix(ig)))/ & (zlev(ig,lmix(ig)+1)-zlev(ig,lmix(ig)))*zmix(ig) + & fraca(ig, lmix(ig)) - zlev(ig, lmix(ig))*(fraca(ig,lmix(ig)+1)-fraca(ig & ,lmix(ig)))/(zlev(ig,lmix(ig)+1)-zlev(ig,lmix(ig))) END DO DO l = 2, nlay DO ig = 1, ngrid IF (larg_cons(ig,l)>1.) THEN IF (l>lmix(ig)) THEN ! test IF (zmax(ig)-zmix(ig)<1.E-10) THEN ! print*,'pb xxx' xxx(ig, l) = (lmaxa(ig)+1.-l)/(lmaxa(ig)+1.-lmix(ig)) ELSE xxx(ig, l) = (zmax(ig)-zlev(ig,l))/(zmax(ig)-zmix(ig)) END IF IF (idetr==0) THEN fraca(ig, l) = fracazmix(ig) ELSE IF (idetr==1) THEN fraca(ig, l) = fracazmix(ig)*xxx(ig, l) ELSE IF (idetr==2) THEN fraca(ig, l) = fracazmix(ig)*(1.-(1.-xxx(ig,l))**2) ELSE fraca(ig, l) = fracazmix(ig)*xxx(ig, l)**2 END IF ! print*,ig,l,lmix(ig),lmaxa(ig),xxx(ig,l),'LLLLLLL' fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) END IF END IF END DO END DO PRINT *, 'fin calcul fraca' ! print*,'11 OK convect8' ! print*,'Ea3 ',wa_moy ! ------------------------------------------------------------------ ! Calcul de fracd, wd ! somme wa - wd = 0 ! ------------------------------------------------------------------ DO ig = 1, ngrid fm(ig, 1) = 0. fm(ig, nlay+1) = 0. END DO DO l = 2, nlay DO ig = 1, ngrid fm(ig, l) = fraca(ig, l)*wa_moy(ig, l)*rhobarz(ig, l) ! CR:test IF (entr(ig,l-1)<1E-10 .AND. fm(ig,l)>fm(ig,l-1) .AND. l>lmix(ig)) THEN fm(ig, l) = fm(ig, l-1) ! write(1,*)'ajustement fm, l',l END IF ! write(1,*)'ig,l,fm(ig,l)',ig,l,fm(ig,l) ! RC END DO DO ig = 1, ngrid IF (fracd(ig,l)<0.1) THEN abort_message = 'fracd trop petit' CALL abort_physic(modname, abort_message, 1) ELSE ! vitesse descendante "diagnostique" wd(ig, l) = fm(ig, l)/(fracd(ig,l)*rhobarz(ig,l)) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid ! masse(ig,l)=rho(ig,l)*(zlev(ig,l+1)-zlev(ig,l)) masse(ig, l) = (pplev(ig,l)-pplev(ig,l+1))/rg END DO END DO ! print*,'12 OK convect8' ! print*,'WA4 ',wa_moy ! c------------------------------------------------------------------ ! calcul du transport vertical ! ------------------------------------------------------------------ GO TO 4444 ! print*,'XXXXXXXXXXXXXXX ptimestep= ',ptimestep DO l = 2, nlay - 1 DO ig = 1, ngrid IF (fm(ig,l+1)*ptimestep>masse(ig,l) .AND. fm(ig,l+1)*ptimestep>masse( & ig,l+1)) THEN ! print*,'WARN!!! FM>M ig=',ig,' l=',l,' FM=' ! s ,fm(ig,l+1)*ptimestep ! s ,' M=',masse(ig,l),masse(ig,l+1) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (entr(ig,l)*ptimestep>masse(ig,l)) THEN ! print*,'WARN!!! E>M ig=',ig,' l=',l,' E==' ! s ,entr(ig,l)*ptimestep ! s ,' M=',masse(ig,l) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (.NOT. fm(ig,l)>=0. .OR. .NOT. fm(ig,l)<=10.) THEN ! print*,'WARN!!! fm exagere ig=',ig,' l=',l ! s ,' FM=',fm(ig,l) END IF IF (.NOT. masse(ig,l)>=1.E-10 .OR. .NOT. masse(ig,l)<=1.E4) THEN ! print*,'WARN!!! masse exagere ig=',ig,' l=',l ! s ,' M=',masse(ig,l) ! print*,'rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l)', ! s rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l) ! print*,'zlev(ig,l+1),zlev(ig,l)' ! s ,zlev(ig,l+1),zlev(ig,l) ! print*,'pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1)' ! s ,pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1) END IF IF (.NOT. entr(ig,l)>=0. .OR. .NOT. entr(ig,l)<=10.) THEN ! print*,'WARN!!! entr exagere ig=',ig,' l=',l ! s ,' E=',entr(ig,l) END IF END DO END DO 4444 CONTINUE ! CR:redefinition du entr DO l = 1, nlay DO ig = 1, ngrid detr(ig, l) = fm(ig, l) + entr(ig, l) - fm(ig, l+1) IF (detr(ig,l)<0.) THEN entr(ig, l) = entr(ig, l) - detr(ig, l) detr(ig, l) = 0. ! print*,'WARNING !!! detrainement negatif ',ig,l END IF END DO END DO ! RC IF (w2di==1) THEN fm0 = fm0 + ptimestep*(fm-fm0)/tho entr0 = entr0 + ptimestep*(entr-entr0)/tho ELSE fm0 = fm entr0 = entr END IF IF (1==1) THEN CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zh, zdhadj, & zha) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zo, pdoadj, & zoa) ELSE CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zh, & zdhadj, zha) CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zo, & pdoadj, zoa) END IF IF (1==0) THEN CALL dvthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zmax, & zu, zv, pduadj, pdvadj, zua, zva) ELSE CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zu, pduadj, & zua) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zv, pdvadj, & zva) END IF DO l = 1, nlay DO ig = 1, ngrid zf = 0.5*(fracc(ig,l)+fracc(ig,l+1)) zf2 = zf/(1.-zf) thetath2(ig, l) = zf2*(zha(ig,l)-zh(ig,l))**2 wth2(ig, l) = zf2*(0.5*(wa_moy(ig,l)+wa_moy(ig,l+1)))**2 END DO END DO ! print*,'13 OK convect8' ! print*,'WA5 ',wa_moy DO l = 1, nlay DO ig = 1, ngrid pdtadj(ig, l) = zdhadj(ig, l)*zpspsk(ig, l) END DO END DO ! do l=1,nlay ! do ig=1,ngrid ! if(abs(pdtadj(ig,l))*86400..gt.500.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdtadj=',pdtadj(ig,l) ! endif ! if(abs(pdoadj(ig,l))*86400..gt.1.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdoadj=',pdoadj(ig,l) ! endif ! enddo ! enddo ! print*,'14 OK convect8' ! ------------------------------------------------------------------ ! Calculs pour les sorties ! ------------------------------------------------------------------ IF (sorties) THEN DO l = 1, nlay DO ig = 1, ngrid zla(ig, l) = (1.-fracd(ig,l))*zmax(ig) zld(ig, l) = fracd(ig, l)*zmax(ig) IF (1.-fracd(ig,l)>1.E-10) zwa(ig, l) = wd(ig, l)*fracd(ig, l)/ & (1.-fracd(ig,l)) END DO END DO ! deja fait ! do l=1,nlay ! do ig=1,ngrid ! detr(ig,l)=fm(ig,l)+entr(ig,l)-fm(ig,l+1) ! if (detr(ig,l).lt.0.) then ! entr(ig,l)=entr(ig,l)-detr(ig,l) ! detr(ig,l)=0. ! print*,'WARNING !!! detrainement negatif ',ig,l ! endif ! enddo ! enddo ! print*,'15 OK convect8' ! #define und GO TO 123 #ifdef und CALL writeg1d(1, nlay, wd, 'wd ', 'wd ') CALL writeg1d(1, nlay, zwa, 'wa ', 'wa ') CALL writeg1d(1, nlay, fracd, 'fracd ', 'fracd ') CALL writeg1d(1, nlay, fraca, 'fraca ', 'fraca ') CALL writeg1d(1, nlay, wa_moy, 'wam ', 'wam ') CALL writeg1d(1, nlay, zla, 'la ', 'la ') CALL writeg1d(1, nlay, zld, 'ld ', 'ld ') CALL writeg1d(1, nlay, pt, 'pt ', 'pt ') CALL writeg1d(1, nlay, zh, 'zh ', 'zh ') CALL writeg1d(1, nlay, zha, 'zha ', 'zha ') CALL writeg1d(1, nlay, zu, 'zu ', 'zu ') CALL writeg1d(1, nlay, zv, 'zv ', 'zv ') CALL writeg1d(1, nlay, zo, 'zo ', 'zo ') CALL writeg1d(1, nlay, wh, 'wh ', 'wh ') CALL writeg1d(1, nlay, wu, 'wu ', 'wu ') CALL writeg1d(1, nlay, wv, 'wv ', 'wv ') CALL writeg1d(1, nlay, wo, 'w15uo ', 'wXo ') CALL writeg1d(1, nlay, zdhadj, 'zdhadj ', 'zdhadj ') CALL writeg1d(1, nlay, pduadj, 'pduadj ', 'pduadj ') CALL writeg1d(1, nlay, pdvadj, 'pdvadj ', 'pdvadj ') CALL writeg1d(1, nlay, pdoadj, 'pdoadj ', 'pdoadj ') CALL writeg1d(1, nlay, entr, 'entr ', 'entr ') CALL writeg1d(1, nlay, detr, 'detr ', 'detr ') CALL writeg1d(1, nlay, fm, 'fm ', 'fm ') CALL writeg1d(1, nlay, pdtadj, 'pdtadj ', 'pdtadj ') CALL writeg1d(1, nlay, pplay, 'pplay ', 'pplay ') CALL writeg1d(1, nlay, pplev, 'pplev ', 'pplev ') ! recalcul des flux en diagnostique... ! print*,'PAS DE TEMPS ',ptimestep CALL dt2f(pplev, pplay, pt, pdtadj, wh) CALL writeg1d(1, nlay, wh, 'wh2 ', 'wh2 ') #endif 123 CONTINUE END IF ! if(wa_moy(1,4).gt.1.e-10) stop ! print*,'19 OK convect8' RETURN END SUBROUTINE thermcell SUBROUTINE dqthermcell(ngrid, nlay, ptimestep, fm, entr, masse, q, dq, qa) USE dimphy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! calcul du dq/dt une fois qu'on connait les ascendances ! ======================================================================= include "dimensions.h" ! ccc#include "dimphy.h" INTEGER ngrid, nlay REAL ptimestep REAL masse(ngrid, nlay), fm(ngrid, nlay+1) REAL entr(ngrid, nlay) REAL q(ngrid, nlay) REAL dq(ngrid, nlay) REAL qa(klon, klev), detr(klon, klev), wqd(klon, klev+1) INTEGER ig, k ! calcul du detrainement DO k = 1, nlay DO ig = 1, ngrid detr(ig, k) = fm(ig, k) - fm(ig, k+1) + entr(ig, k) ! test IF (detr(ig,k)<0.) THEN entr(ig, k) = entr(ig, k) - detr(ig, k) detr(ig, k) = 0. ! print*,'detr2<0!!!','ig=',ig,'k=',k,'f=',fm(ig,k), ! s 'f+1=',fm(ig,k+1),'e=',entr(ig,k),'d=',detr(ig,k) END IF IF (fm(ig,k+1)<0.) THEN ! print*,'fm2<0!!!' END IF IF (entr(ig,k)<0.) THEN ! print*,'entr2<0!!!' END IF END DO END DO ! calcul de la valeur dans les ascendances DO ig = 1, ngrid qa(ig, 1) = q(ig, 1) END DO DO k = 2, nlay DO ig = 1, ngrid IF ((fm(ig,k+1)+detr(ig,k))*ptimestep>1.E-5*masse(ig,k)) THEN qa(ig, k) = (fm(ig,k)*qa(ig,k-1)+entr(ig,k)*q(ig,k))/ & (fm(ig,k+1)+detr(ig,k)) ELSE qa(ig, k) = q(ig, k) END IF IF (qa(ig,k)<0.) THEN ! print*,'qa<0!!!' END IF IF (q(ig,k)<0.) THEN ! print*,'q<0!!!' END IF END DO END DO DO k = 2, nlay DO ig = 1, ngrid ! wqd(ig,k)=fm(ig,k)*0.5*(q(ig,k-1)+q(ig,k)) wqd(ig, k) = fm(ig, k)*q(ig, k) IF (wqd(ig,k)<0.) THEN ! print*,'wqd<0!!!' END IF END DO END DO DO ig = 1, ngrid wqd(ig, 1) = 0. wqd(ig, nlay+1) = 0. END DO DO k = 1, nlay DO ig = 1, ngrid dq(ig, k) = (detr(ig,k)*qa(ig,k)-entr(ig,k)*q(ig,k)-wqd(ig,k)+wqd(ig,k+ & 1))/masse(ig, k) ! if (dq(ig,k).lt.0.) then ! print*,'dq<0!!!' ! endif END DO END DO RETURN END SUBROUTINE dqthermcell SUBROUTINE dvthermcell(ngrid, nlay, ptimestep, fm, entr, masse, fraca, larga, & u, v, du, dv, ua, va) USE dimphy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! calcul du dq/dt une fois qu'on connait les ascendances ! ======================================================================= include "dimensions.h" ! ccc#include "dimphy.h" INTEGER ngrid, nlay REAL ptimestep REAL masse(ngrid, nlay), fm(ngrid, nlay+1) REAL fraca(ngrid, nlay+1) REAL larga(ngrid) REAL entr(ngrid, nlay) REAL u(ngrid, nlay) REAL ua(ngrid, nlay) REAL du(ngrid, nlay) REAL v(ngrid, nlay) REAL va(ngrid, nlay) REAL dv(ngrid, nlay) REAL qa(klon, klev), detr(klon, klev) REAL wvd(klon, klev+1), wud(klon, klev+1) REAL gamma0, gamma(klon, klev+1) REAL dua, dva INTEGER iter INTEGER ig, k ! calcul du detrainement DO k = 1, nlay DO ig = 1, ngrid detr(ig, k) = fm(ig, k) - fm(ig, k+1) + entr(ig, k) END DO END DO ! calcul de la valeur dans les ascendances DO ig = 1, ngrid ua(ig, 1) = u(ig, 1) va(ig, 1) = v(ig, 1) END DO DO k = 2, nlay DO ig = 1, ngrid IF ((fm(ig,k+1)+detr(ig,k))*ptimestep>1.E-5*masse(ig,k)) THEN ! On itère sur la valeur du coeff de freinage. ! gamma0=rho(ig,k)*(zlev(ig,k+1)-zlev(ig,k)) gamma0 = masse(ig, k)*sqrt(0.5*(fraca(ig,k+1)+fraca(ig, & k)))*0.5/larga(ig) ! gamma0=0. ! la première fois on multiplie le coefficient de freinage ! par le module du vent dans la couche en dessous. dua = ua(ig, k-1) - u(ig, k-1) dva = va(ig, k-1) - v(ig, k-1) DO iter = 1, 5 gamma(ig, k) = gamma0*sqrt(dua**2+dva**2) ua(ig, k) = (fm(ig,k)*ua(ig,k-1)+(entr(ig,k)+gamma(ig, & k))*u(ig,k))/(fm(ig,k+1)+detr(ig,k)+gamma(ig,k)) va(ig, k) = (fm(ig,k)*va(ig,k-1)+(entr(ig,k)+gamma(ig, & k))*v(ig,k))/(fm(ig,k+1)+detr(ig,k)+gamma(ig,k)) ! print*,k,ua(ig,k),va(ig,k),u(ig,k),v(ig,k),dua,dva dua = ua(ig, k) - u(ig, k) dva = va(ig, k) - v(ig, k) END DO ELSE ua(ig, k) = u(ig, k) va(ig, k) = v(ig, k) gamma(ig, k) = 0. END IF END DO END DO DO k = 2, nlay DO ig = 1, ngrid wud(ig, k) = fm(ig, k)*u(ig, k) wvd(ig, k) = fm(ig, k)*v(ig, k) END DO END DO DO ig = 1, ngrid wud(ig, 1) = 0. wud(ig, nlay+1) = 0. wvd(ig, 1) = 0. wvd(ig, nlay+1) = 0. END DO DO k = 1, nlay DO ig = 1, ngrid du(ig, k) = ((detr(ig,k)+gamma(ig,k))*ua(ig,k)-(entr(ig,k)+gamma(ig, & k))*u(ig,k)-wud(ig,k)+wud(ig,k+1))/masse(ig, k) dv(ig, k) = ((detr(ig,k)+gamma(ig,k))*va(ig,k)-(entr(ig,k)+gamma(ig, & k))*v(ig,k)-wvd(ig,k)+wvd(ig,k+1))/masse(ig, k) END DO END DO RETURN END SUBROUTINE dvthermcell SUBROUTINE dqthermcell2(ngrid, nlay, ptimestep, fm, entr, masse, frac, q, dq, & qa) USE dimphy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! calcul du dq/dt une fois qu'on connait les ascendances ! ======================================================================= include "dimensions.h" ! ccc#include "dimphy.h" INTEGER ngrid, nlay REAL ptimestep REAL masse(ngrid, nlay), fm(ngrid, nlay+1) REAL entr(ngrid, nlay), frac(ngrid, nlay) REAL q(ngrid, nlay) REAL dq(ngrid, nlay) REAL qa(klon, klev), detr(klon, klev), wqd(klon, klev+1) REAL qe(klon, klev), zf, zf2 INTEGER ig, k ! calcul du detrainement DO k = 1, nlay DO ig = 1, ngrid detr(ig, k) = fm(ig, k) - fm(ig, k+1) + entr(ig, k) END DO END DO ! calcul de la valeur dans les ascendances DO ig = 1, ngrid qa(ig, 1) = q(ig, 1) qe(ig, 1) = q(ig, 1) END DO DO k = 2, nlay DO ig = 1, ngrid IF ((fm(ig,k+1)+detr(ig,k))*ptimestep>1.E-5*masse(ig,k)) THEN zf = 0.5*(frac(ig,k)+frac(ig,k+1)) zf2 = 1./(1.-zf) qa(ig, k) = (fm(ig,k)*qa(ig,k-1)+zf2*entr(ig,k)*q(ig,k))/ & (fm(ig,k+1)+detr(ig,k)+entr(ig,k)*zf*zf2) qe(ig, k) = (q(ig,k)-zf*qa(ig,k))*zf2 ELSE qa(ig, k) = q(ig, k) qe(ig, k) = q(ig, k) END IF END DO END DO DO k = 2, nlay DO ig = 1, ngrid ! wqd(ig,k)=fm(ig,k)*0.5*(q(ig,k-1)+q(ig,k)) wqd(ig, k) = fm(ig, k)*qe(ig, k) END DO END DO DO ig = 1, ngrid wqd(ig, 1) = 0. wqd(ig, nlay+1) = 0. END DO DO k = 1, nlay DO ig = 1, ngrid dq(ig, k) = (detr(ig,k)*qa(ig,k)-entr(ig,k)*qe(ig,k)-wqd(ig,k)+wqd(ig,k & +1))/masse(ig, k) END DO END DO RETURN END SUBROUTINE dqthermcell2 SUBROUTINE dvthermcell2(ngrid, nlay, ptimestep, fm, entr, masse, fraca, & larga, u, v, du, dv, ua, va) USE dimphy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! calcul du dq/dt une fois qu'on connait les ascendances ! ======================================================================= include "dimensions.h" ! ccc#include "dimphy.h" INTEGER ngrid, nlay REAL ptimestep REAL masse(ngrid, nlay), fm(ngrid, nlay+1) REAL fraca(ngrid, nlay+1) REAL larga(ngrid) REAL entr(ngrid, nlay) REAL u(ngrid, nlay) REAL ua(ngrid, nlay) REAL du(ngrid, nlay) REAL v(ngrid, nlay) REAL va(ngrid, nlay) REAL dv(ngrid, nlay) REAL qa(klon, klev), detr(klon, klev), zf, zf2 REAL wvd(klon, klev+1), wud(klon, klev+1) REAL gamma0, gamma(klon, klev+1) REAL ue(klon, klev), ve(klon, klev) REAL dua, dva INTEGER iter INTEGER ig, k ! calcul du detrainement DO k = 1, nlay DO ig = 1, ngrid detr(ig, k) = fm(ig, k) - fm(ig, k+1) + entr(ig, k) END DO END DO ! calcul de la valeur dans les ascendances DO ig = 1, ngrid ua(ig, 1) = u(ig, 1) va(ig, 1) = v(ig, 1) ue(ig, 1) = u(ig, 1) ve(ig, 1) = v(ig, 1) END DO DO k = 2, nlay DO ig = 1, ngrid IF ((fm(ig,k+1)+detr(ig,k))*ptimestep>1.E-5*masse(ig,k)) THEN ! On itère sur la valeur du coeff de freinage. ! gamma0=rho(ig,k)*(zlev(ig,k+1)-zlev(ig,k)) gamma0 = masse(ig, k)*sqrt(0.5*(fraca(ig,k+1)+fraca(ig, & k)))*0.5/larga(ig)*1. ! s *0.5 ! gamma0=0. zf = 0.5*(fraca(ig,k)+fraca(ig,k+1)) zf = 0. zf2 = 1./(1.-zf) ! la première fois on multiplie le coefficient de freinage ! par le module du vent dans la couche en dessous. dua = ua(ig, k-1) - u(ig, k-1) dva = va(ig, k-1) - v(ig, k-1) DO iter = 1, 5 ! On choisit une relaxation lineaire. gamma(ig, k) = gamma0 ! On choisit une relaxation quadratique. gamma(ig, k) = gamma0*sqrt(dua**2+dva**2) ua(ig, k) = (fm(ig,k)*ua(ig,k-1)+(zf2*entr(ig,k)+gamma(ig, & k))*u(ig,k))/(fm(ig,k+1)+detr(ig,k)+entr(ig,k)*zf*zf2+gamma(ig,k) & ) va(ig, k) = (fm(ig,k)*va(ig,k-1)+(zf2*entr(ig,k)+gamma(ig, & k))*v(ig,k))/(fm(ig,k+1)+detr(ig,k)+entr(ig,k)*zf*zf2+gamma(ig,k) & ) ! print*,k,ua(ig,k),va(ig,k),u(ig,k),v(ig,k),dua,dva dua = ua(ig, k) - u(ig, k) dva = va(ig, k) - v(ig, k) ue(ig, k) = (u(ig,k)-zf*ua(ig,k))*zf2 ve(ig, k) = (v(ig,k)-zf*va(ig,k))*zf2 END DO ELSE ua(ig, k) = u(ig, k) va(ig, k) = v(ig, k) ue(ig, k) = u(ig, k) ve(ig, k) = v(ig, k) gamma(ig, k) = 0. END IF END DO END DO DO k = 2, nlay DO ig = 1, ngrid wud(ig, k) = fm(ig, k)*ue(ig, k) wvd(ig, k) = fm(ig, k)*ve(ig, k) END DO END DO DO ig = 1, ngrid wud(ig, 1) = 0. wud(ig, nlay+1) = 0. wvd(ig, 1) = 0. wvd(ig, nlay+1) = 0. END DO DO k = 1, nlay DO ig = 1, ngrid du(ig, k) = ((detr(ig,k)+gamma(ig,k))*ua(ig,k)-(entr(ig,k)+gamma(ig, & k))*ue(ig,k)-wud(ig,k)+wud(ig,k+1))/masse(ig, k) dv(ig, k) = ((detr(ig,k)+gamma(ig,k))*va(ig,k)-(entr(ig,k)+gamma(ig, & k))*ve(ig,k)-wvd(ig,k)+wvd(ig,k+1))/masse(ig, k) END DO END DO RETURN END SUBROUTINE dvthermcell2 SUBROUTINE thermcell_sec(ngrid, nlay, ptimestep, pplay, pplev, pphi, zlev, & pu, pv, pt, po, pduadj, pdvadj, pdtadj, pdoadj, fm0, entr0 & ! s ! ,pu_therm,pv_therm , r_aspect, l_mix, w2di, tho) USE dimphy IMPLICIT NONE ! ======================================================================= ! Calcul du transport verticale dans la couche limite en presence ! de "thermiques" explicitement representes ! Réécriture à partir d'un listing papier à Habas, le 14/02/00 ! le thermique est supposé homogène et dissipé par mélange avec ! son environnement. la longueur l_mix contrôle l'efficacité du ! mélange ! Le calcul du transport des différentes espèces se fait en prenant ! en compte: ! 1. un flux de masse montant ! 2. un flux de masse descendant ! 3. un entrainement ! 4. un detrainement ! ======================================================================= ! ----------------------------------------------------------------------- ! declarations: ! ------------- include "dimensions.h" ! ccc#include "dimphy.h" include "YOMCST.h" ! arguments: ! ---------- INTEGER ngrid, nlay, w2di REAL tho REAL ptimestep, l_mix, r_aspect REAL pt(ngrid, nlay), pdtadj(ngrid, nlay) REAL pu(ngrid, nlay), pduadj(ngrid, nlay) REAL pv(ngrid, nlay), pdvadj(ngrid, nlay) REAL po(ngrid, nlay), pdoadj(ngrid, nlay) REAL pplay(ngrid, nlay), pplev(ngrid, nlay+1) REAL pphi(ngrid, nlay) INTEGER idetr SAVE idetr DATA idetr/3/ !$OMP THREADPRIVATE(idetr) ! local: ! ------ INTEGER ig, k, l, lmaxa(klon), lmix(klon) REAL zsortie1d(klon) ! CR: on remplace lmax(klon,klev+1) INTEGER lmax(klon), lmin(klon), lentr(klon) REAL linter(klon) REAL zmix(klon), fracazmix(klon) ! RC REAL zmax(klon), zw, zz, zw2(klon, klev+1), ztva(klon, klev), zzz REAL zlev(klon, klev+1), zlay(klon, klev) REAL zh(klon, klev), zdhadj(klon, klev) REAL ztv(klon, klev) REAL zu(klon, klev), zv(klon, klev), zo(klon, klev) REAL wh(klon, klev+1) REAL wu(klon, klev+1), wv(klon, klev+1), wo(klon, klev+1) REAL zla(klon, klev+1) REAL zwa(klon, klev+1) REAL zld(klon, klev+1) REAL zwd(klon, klev+1) REAL zsortie(klon, klev) REAL zva(klon, klev) REAL zua(klon, klev) REAL zoa(klon, klev) REAL zha(klon, klev) REAL wa_moy(klon, klev+1) REAL fraca(klon, klev+1) REAL fracc(klon, klev+1) REAL zf, zf2 REAL thetath2(klon, klev), wth2(klon, klev) ! common/comtherm/thetath2,wth2 REAL count_time INTEGER ialt LOGICAL sorties REAL rho(klon, klev), rhobarz(klon, klev+1), masse(klon, klev) REAL zpspsk(klon, klev) ! real wmax(klon,klev),wmaxa(klon) REAL wmax(klon), wmaxa(klon) REAL wa(klon, klev, klev+1) REAL wd(klon, klev+1) REAL larg_part(klon, klev, klev+1) REAL fracd(klon, klev+1) REAL xxx(klon, klev+1) REAL larg_cons(klon, klev+1) REAL larg_detr(klon, klev+1) REAL fm0(klon, klev+1), entr0(klon, klev), detr(klon, klev) REAL pu_therm(klon, klev), pv_therm(klon, klev) REAL fm(klon, klev+1), entr(klon, klev) REAL fmc(klon, klev+1) ! CR:nouvelles variables REAL f_star(klon, klev+1), entr_star(klon, klev) REAL entr_star_tot(klon), entr_star2(klon) REAL f(klon), f0(klon) REAL zlevinter(klon) LOGICAL first DATA first/.FALSE./ SAVE first !$OMP THREADPRIVATE(first) ! RC CHARACTER *2 str2 CHARACTER *10 str10 CHARACTER (LEN=20) :: modname = 'thermcell_sec' CHARACTER (LEN=80) :: abort_message LOGICAL vtest(klon), down EXTERNAL scopy INTEGER ncorrec, ll SAVE ncorrec DATA ncorrec/0/ !$OMP THREADPRIVATE(ncorrec) ! ----------------------------------------------------------------------- ! initialisation: ! --------------- sorties = .TRUE. IF (ngrid/=klon) THEN PRINT * PRINT *, 'STOP dans convadj' PRINT *, 'ngrid =', ngrid PRINT *, 'klon =', klon END IF ! ----------------------------------------------------------------------- ! incrementation eventuelle de tendances precedentes: ! --------------------------------------------------- ! print*,'0 OK convect8' DO l = 1, nlay DO ig = 1, ngrid zpspsk(ig, l) = (pplay(ig,l)/pplev(ig,1))**rkappa zh(ig, l) = pt(ig, l)/zpspsk(ig, l) zu(ig, l) = pu(ig, l) zv(ig, l) = pv(ig, l) zo(ig, l) = po(ig, l) ztv(ig, l) = zh(ig, l)*(1.+0.61*zo(ig,l)) END DO END DO ! print*,'1 OK convect8' ! -------------------- ! + + + + + + + + + + + ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz ! wh,wt,wo ... ! + + + + + + + + + + + zh,zu,zv,zo,rho ! -------------------- zlev(1) ! \\\\\\\\\\\\\\\\\\\\ ! ----------------------------------------------------------------------- ! Calcul des altitudes des couches ! ----------------------------------------------------------------------- DO l = 2, nlay DO ig = 1, ngrid zlev(ig, l) = 0.5*(pphi(ig,l)+pphi(ig,l-1))/rg END DO END DO DO ig = 1, ngrid zlev(ig, 1) = 0. zlev(ig, nlay+1) = (2.*pphi(ig,klev)-pphi(ig,klev-1))/rg END DO DO l = 1, nlay DO ig = 1, ngrid zlay(ig, l) = pphi(ig, l)/rg END DO END DO ! print*,'2 OK convect8' ! ----------------------------------------------------------------------- ! Calcul des densites ! ----------------------------------------------------------------------- DO l = 1, nlay DO ig = 1, ngrid rho(ig, l) = pplay(ig, l)/(zpspsk(ig,l)*rd*zh(ig,l)) END DO END DO DO l = 2, nlay DO ig = 1, ngrid rhobarz(ig, l) = 0.5*(rho(ig,l)+rho(ig,l-1)) END DO END DO DO k = 1, nlay DO l = 1, nlay + 1 DO ig = 1, ngrid wa(ig, k, l) = 0. END DO END DO END DO ! print*,'3 OK convect8' ! ------------------------------------------------------------------ ! Calcul de w2, quarre de w a partir de la cape ! a partir de w2, on calcule wa, vitesse de l'ascendance ! ATTENTION: Dans cette version, pour cause d'economie de memoire, ! w2 est stoke dans wa ! ATTENTION: dans convect8, on n'utilise le calcule des wa ! independants par couches que pour calculer l'entrainement ! a la base et la hauteur max de l'ascendance. ! Indicages: ! l'ascendance provenant du niveau k traverse l'interface l avec ! une vitesse wa(k,l). ! -------------------- ! + + + + + + + + + + ! wa(k,l) ---- -------------------- l ! /\ ! /||\ + + + + + + + + + + ! || ! || -------------------- ! || ! || + + + + + + + + + + ! || ! || -------------------- ! ||__ ! |___ + + + + + + + + + + k ! -------------------- ! ------------------------------------------------------------------ ! CR: ponderation entrainement des couches instables ! def des entr_star tels que entr=f*entr_star DO l = 1, klev DO ig = 1, ngrid entr_star(ig, l) = 0. END DO END DO ! determination de la longueur de la couche d entrainement DO ig = 1, ngrid lentr(ig) = 1 END DO ! on ne considere que les premieres couches instables DO k = nlay - 2, 1, -1 DO ig = 1, ngrid IF (ztv(ig,k)>ztv(ig,k+1) .AND. ztv(ig,k+1)<=ztv(ig,k+2)) THEN lentr(ig) = k END IF END DO END DO ! determination du lmin: couche d ou provient le thermique DO ig = 1, ngrid lmin(ig) = 1 END DO DO ig = 1, ngrid DO l = nlay, 2, -1 IF (ztv(ig,l-1)>ztv(ig,l)) THEN lmin(ig) = l - 1 END IF END DO END DO ! definition de l'entrainement des couches DO l = 1, klev - 1 DO ig = 1, ngrid IF (ztv(ig,l)>ztv(ig,l+1) .AND. l>=lmin(ig) .AND. l<=lentr(ig)) THEN entr_star(ig, l) = (ztv(ig,l)-ztv(ig,l+1))** & ! s ! (zlev(ig,l+1)-zlev(ig,l)) sqrt(zlev(ig,l+1)) END IF END DO END DO ! pas de thermique si couche 1 stable DO ig = 1, ngrid IF (lmin(ig)>1) THEN DO l = 1, klev entr_star(ig, l) = 0. END DO END IF END DO ! calcul de l entrainement total DO ig = 1, ngrid entr_star_tot(ig) = 0. END DO DO ig = 1, ngrid DO k = 1, klev entr_star_tot(ig) = entr_star_tot(ig) + entr_star(ig, k) END DO END DO ! print*,'fin calcul entr_star' DO k = 1, klev DO ig = 1, ngrid ztva(ig, k) = ztv(ig, k) END DO END DO ! RC ! print*,'7 OK convect8' DO k = 1, klev + 1 DO ig = 1, ngrid zw2(ig, k) = 0. fmc(ig, k) = 0. ! CR f_star(ig, k) = 0. ! RC larg_cons(ig, k) = 0. larg_detr(ig, k) = 0. wa_moy(ig, k) = 0. END DO END DO ! print*,'8 OK convect8' DO ig = 1, ngrid linter(ig) = 1. lmaxa(ig) = 1 lmix(ig) = 1 wmaxa(ig) = 0. END DO ! CR: DO l = 1, nlay - 2 DO ig = 1, ngrid IF (ztv(ig,l)>ztv(ig,l+1) .AND. entr_star(ig,l)>1.E-10 .AND. & zw2(ig,l)<1E-10) THEN f_star(ig, l+1) = entr_star(ig, l) ! test:calcul de dteta zw2(ig, l+1) = 2.*rg*(ztv(ig,l)-ztv(ig,l+1))/ztv(ig, l+1)* & (zlev(ig,l+1)-zlev(ig,l))*0.4*pphi(ig, l)/(pphi(ig,l+1)-pphi(ig,l)) larg_detr(ig, l) = 0. ELSE IF ((zw2(ig,l)>=1E-10) .AND. (f_star(ig,l)+entr_star(ig, & l)>1.E-10)) THEN f_star(ig, l+1) = f_star(ig, l) + entr_star(ig, l) ztva(ig, l) = (f_star(ig,l)*ztva(ig,l-1)+entr_star(ig,l)*ztv(ig,l))/ & f_star(ig, l+1) zw2(ig, l+1) = zw2(ig, l)*(f_star(ig,l)/f_star(ig,l+1))**2 + & 2.*rg*(ztva(ig,l)-ztv(ig,l))/ztv(ig, l)*(zlev(ig,l+1)-zlev(ig,l)) END IF ! determination de zmax continu par interpolation lineaire IF (zw2(ig,l+1)<0.) THEN ! test IF (abs(zw2(ig,l+1)-zw2(ig,l))<1E-10) THEN ! print*,'pb linter' END IF linter(ig) = (l*(zw2(ig,l+1)-zw2(ig,l))-zw2(ig,l))/(zw2(ig,l+1)-zw2( & ig,l)) zw2(ig, l+1) = 0. lmaxa(ig) = l ELSE IF (zw2(ig,l+1)<0.) THEN ! print*,'pb1 zw2<0' END IF wa_moy(ig, l+1) = sqrt(zw2(ig,l+1)) END IF IF (wa_moy(ig,l+1)>wmaxa(ig)) THEN ! lmix est le niveau de la couche ou w (wa_moy) est maximum lmix(ig) = l + 1 wmaxa(ig) = wa_moy(ig, l+1) END IF END DO END DO ! print*,'fin calcul zw2' ! Calcul de la couche correspondant a la hauteur du thermique DO ig = 1, ngrid lmax(ig) = lentr(ig) END DO DO ig = 1, ngrid DO l = nlay, lentr(ig) + 1, -1 IF (zw2(ig,l)<=1.E-10) THEN lmax(ig) = l - 1 END IF END DO END DO ! pas de thermique si couche 1 stable DO ig = 1, ngrid IF (lmin(ig)>1) THEN lmax(ig) = 1 lmin(ig) = 1 END IF END DO ! Determination de zw2 max DO ig = 1, ngrid wmax(ig) = 0. END DO DO l = 1, nlay DO ig = 1, ngrid IF (l<=lmax(ig)) THEN IF (zw2(ig,l)<0.) THEN ! print*,'pb2 zw2<0' END IF zw2(ig, l) = sqrt(zw2(ig,l)) wmax(ig) = max(wmax(ig), zw2(ig,l)) ELSE zw2(ig, l) = 0. END IF END DO END DO ! Longueur caracteristique correspondant a la hauteur des thermiques. DO ig = 1, ngrid zmax(ig) = 0. zlevinter(ig) = zlev(ig, 1) END DO DO ig = 1, ngrid ! calcul de zlevinter zlevinter(ig) = (zlev(ig,lmax(ig)+1)-zlev(ig,lmax(ig)))*linter(ig) + & zlev(ig, lmax(ig)) - lmax(ig)*(zlev(ig,lmax(ig)+1)-zlev(ig,lmax(ig))) zmax(ig) = max(zmax(ig), zlevinter(ig)-zlev(ig,lmin(ig))) END DO ! print*,'avant fermeture' ! Fermeture,determination de f DO ig = 1, ngrid entr_star2(ig) = 0. END DO DO ig = 1, ngrid IF (entr_star_tot(ig)<1.E-10) THEN f(ig) = 0. ELSE DO k = lmin(ig), lentr(ig) entr_star2(ig) = entr_star2(ig) + entr_star(ig, k)**2/(rho(ig,k)*( & zlev(ig,k+1)-zlev(ig,k))) END DO ! Nouvelle fermeture f(ig) = wmax(ig)/(max(500.,zmax(ig))*r_aspect*entr_star2(ig))* & entr_star_tot(ig) ! test ! if (first) then ! f(ig)=f(ig)+(f0(ig)-f(ig))*exp(-ptimestep/zmax(ig) ! s *wmax(ig)) ! endif END IF ! f0(ig)=f(ig) ! first=.true. END DO ! print*,'apres fermeture' ! Calcul de l'entrainement DO k = 1, klev DO ig = 1, ngrid entr(ig, k) = f(ig)*entr_star(ig, k) END DO END DO ! CR:test pour entrainer moins que la masse DO ig = 1, ngrid DO l = 1, lentr(ig) IF ((entr(ig,l)*ptimestep)>(0.9*masse(ig,l))) THEN entr(ig, l+1) = entr(ig, l+1) + entr(ig, l) - & 0.9*masse(ig, l)/ptimestep entr(ig, l) = 0.9*masse(ig, l)/ptimestep END IF END DO END DO ! CR: fin test ! Calcul des flux DO ig = 1, ngrid DO l = 1, lmax(ig) - 1 fmc(ig, l+1) = fmc(ig, l) + entr(ig, l) END DO END DO ! RC ! print*,'9 OK convect8' ! print*,'WA1 ',wa_moy ! determination de l'indice du debut de la mixed layer ou w decroit ! calcul de la largeur de chaque ascendance dans le cas conservatif. ! dans ce cas simple, on suppose que la largeur de l'ascendance provenant ! d'une couche est égale à la hauteur de la couche alimentante. ! La vitesse maximale dans l'ascendance est aussi prise comme estimation ! de la vitesse d'entrainement horizontal dans la couche alimentante. DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmaxa(ig)) THEN zw = max(wa_moy(ig,l), 1.E-10) larg_cons(ig, l) = zmax(ig)*r_aspect*fmc(ig, l)/(rhobarz(ig,l)*zw) END IF END DO END DO DO l = 2, nlay DO ig = 1, ngrid IF (l<=lmaxa(ig)) THEN ! if (idetr.eq.0) then ! cette option est finalement en dur. IF ((l_mix*zlev(ig,l))<0.) THEN ! print*,'pb l_mix*zlev<0' END IF ! CR: test: nouvelle def de lambda ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) IF (zw2(ig,l)>1.E-10) THEN larg_detr(ig, l) = sqrt((l_mix/zw2(ig,l))*zlev(ig,l)) ELSE larg_detr(ig, l) = sqrt(l_mix*zlev(ig,l)) END IF ! RC ! else if (idetr.eq.1) then ! larg_detr(ig,l)=larg_cons(ig,l) ! s *sqrt(l_mix*zlev(ig,l))/larg_cons(ig,lmix(ig)) ! else if (idetr.eq.2) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *sqrt(wa_moy(ig,l)) ! else if (idetr.eq.4) then ! larg_detr(ig,l)=sqrt(l_mix*zlev(ig,l)) ! s *wa_moy(ig,l) ! endif END IF END DO END DO ! print*,'10 OK convect8' ! print*,'WA2 ',wa_moy ! calcul de la fraction de la maille concernée par l'ascendance en tenant ! compte de l'epluchage du thermique. ! CR def de zmix continu (profil parabolique des vitesses) DO ig = 1, ngrid IF (lmix(ig)>1.) THEN ! test IF (((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)))- & (zlev(ig,lmix(ig)+1)))-(zw2(ig,lmix(ig))- & zw2(ig,lmix(ig)+1))*((zlev(ig,lmix(ig)-1))- & (zlev(ig,lmix(ig)))))>1E-10) THEN zmix(ig) = ((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)) & )**2-(zlev(ig,lmix(ig)+1))**2)-(zw2(ig,lmix(ig))-zw2(ig, & lmix(ig)+1))*((zlev(ig,lmix(ig)-1))**2-(zlev(ig,lmix(ig)))**2))/ & (2.*((zw2(ig,lmix(ig)-1)-zw2(ig,lmix(ig)))*((zlev(ig,lmix(ig)))- & (zlev(ig,lmix(ig)+1)))-(zw2(ig,lmix(ig))- & zw2(ig,lmix(ig)+1))*((zlev(ig,lmix(ig)-1))-(zlev(ig,lmix(ig)))))) ELSE zmix(ig) = zlev(ig, lmix(ig)) ! print*,'pb zmix' END IF ELSE zmix(ig) = 0. END IF ! test IF ((zmax(ig)-zmix(ig))<0.) THEN zmix(ig) = 0.99*zmax(ig) ! print*,'pb zmix>zmax' END IF END DO ! calcul du nouveau lmix correspondant DO ig = 1, ngrid DO l = 1, klev IF (zmix(ig)>=zlev(ig,l) .AND. zmix(ig)1.) THEN ! print*,ig,l,lmix(ig),lmaxa(ig),larg_cons(ig,l),' KKK' fraca(ig, l) = (larg_cons(ig,l)-larg_detr(ig,l))/(r_aspect*zmax(ig)) ! test fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) ELSE ! wa_moy(ig,l)=0. fraca(ig, l) = 0. fracc(ig, l) = 0. fracd(ig, l) = 1. END IF END DO END DO ! CR: calcul de fracazmix DO ig = 1, ngrid fracazmix(ig) = (fraca(ig,lmix(ig)+1)-fraca(ig,lmix(ig)))/ & (zlev(ig,lmix(ig)+1)-zlev(ig,lmix(ig)))*zmix(ig) + & fraca(ig, lmix(ig)) - zlev(ig, lmix(ig))*(fraca(ig,lmix(ig)+1)-fraca(ig & ,lmix(ig)))/(zlev(ig,lmix(ig)+1)-zlev(ig,lmix(ig))) END DO DO l = 2, nlay DO ig = 1, ngrid IF (larg_cons(ig,l)>1.) THEN IF (l>lmix(ig)) THEN ! test IF (zmax(ig)-zmix(ig)<1.E-10) THEN ! print*,'pb xxx' xxx(ig, l) = (lmaxa(ig)+1.-l)/(lmaxa(ig)+1.-lmix(ig)) ELSE xxx(ig, l) = (zmax(ig)-zlev(ig,l))/(zmax(ig)-zmix(ig)) END IF IF (idetr==0) THEN fraca(ig, l) = fracazmix(ig) ELSE IF (idetr==1) THEN fraca(ig, l) = fracazmix(ig)*xxx(ig, l) ELSE IF (idetr==2) THEN fraca(ig, l) = fracazmix(ig)*(1.-(1.-xxx(ig,l))**2) ELSE fraca(ig, l) = fracazmix(ig)*xxx(ig, l)**2 END IF ! print*,ig,l,lmix(ig),lmaxa(ig),xxx(ig,l),'LLLLLLL' fraca(ig, l) = max(fraca(ig,l), 0.) fraca(ig, l) = min(fraca(ig,l), 0.5) fracd(ig, l) = 1. - fraca(ig, l) fracc(ig, l) = larg_cons(ig, l)/(r_aspect*zmax(ig)) END IF END IF END DO END DO ! print*,'fin calcul fraca' ! print*,'11 OK convect8' ! print*,'Ea3 ',wa_moy ! ------------------------------------------------------------------ ! Calcul de fracd, wd ! somme wa - wd = 0 ! ------------------------------------------------------------------ DO ig = 1, ngrid fm(ig, 1) = 0. fm(ig, nlay+1) = 0. END DO DO l = 2, nlay DO ig = 1, ngrid fm(ig, l) = fraca(ig, l)*wa_moy(ig, l)*rhobarz(ig, l) ! CR:test IF (entr(ig,l-1)<1E-10 .AND. fm(ig,l)>fm(ig,l-1) .AND. l>lmix(ig)) THEN fm(ig, l) = fm(ig, l-1) ! write(1,*)'ajustement fm, l',l END IF ! write(1,*)'ig,l,fm(ig,l)',ig,l,fm(ig,l) ! RC END DO DO ig = 1, ngrid IF (fracd(ig,l)<0.1) THEN abort_message = 'fracd trop petit' CALL abort_physic(modname, abort_message, 1) ELSE ! vitesse descendante "diagnostique" wd(ig, l) = fm(ig, l)/(fracd(ig,l)*rhobarz(ig,l)) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid ! masse(ig,l)=rho(ig,l)*(zlev(ig,l+1)-zlev(ig,l)) masse(ig, l) = (pplev(ig,l)-pplev(ig,l+1))/rg END DO END DO ! print*,'12 OK convect8' ! print*,'WA4 ',wa_moy ! c------------------------------------------------------------------ ! calcul du transport vertical ! ------------------------------------------------------------------ GO TO 4444 ! print*,'XXXXXXXXXXXXXXX ptimestep= ',ptimestep DO l = 2, nlay - 1 DO ig = 1, ngrid IF (fm(ig,l+1)*ptimestep>masse(ig,l) .AND. fm(ig,l+1)*ptimestep>masse( & ig,l+1)) THEN ! print*,'WARN!!! FM>M ig=',ig,' l=',l,' FM=' ! s ,fm(ig,l+1)*ptimestep ! s ,' M=',masse(ig,l),masse(ig,l+1) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (entr(ig,l)*ptimestep>masse(ig,l)) THEN ! print*,'WARN!!! E>M ig=',ig,' l=',l,' E==' ! s ,entr(ig,l)*ptimestep ! s ,' M=',masse(ig,l) END IF END DO END DO DO l = 1, nlay DO ig = 1, ngrid IF (.NOT. fm(ig,l)>=0. .OR. .NOT. fm(ig,l)<=10.) THEN ! print*,'WARN!!! fm exagere ig=',ig,' l=',l ! s ,' FM=',fm(ig,l) END IF IF (.NOT. masse(ig,l)>=1.E-10 .OR. .NOT. masse(ig,l)<=1.E4) THEN ! print*,'WARN!!! masse exagere ig=',ig,' l=',l ! s ,' M=',masse(ig,l) ! print*,'rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l)', ! s rho(ig,l),pplay(ig,l),zpspsk(ig,l),RD,zh(ig,l) ! print*,'zlev(ig,l+1),zlev(ig,l)' ! s ,zlev(ig,l+1),zlev(ig,l) ! print*,'pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1)' ! s ,pphi(ig,l-1),pphi(ig,l),pphi(ig,l+1) END IF IF (.NOT. entr(ig,l)>=0. .OR. .NOT. entr(ig,l)<=10.) THEN ! print*,'WARN!!! entr exagere ig=',ig,' l=',l ! s ,' E=',entr(ig,l) END IF END DO END DO 4444 CONTINUE ! CR:redefinition du entr DO l = 1, nlay DO ig = 1, ngrid detr(ig, l) = fm(ig, l) + entr(ig, l) - fm(ig, l+1) IF (detr(ig,l)<0.) THEN entr(ig, l) = entr(ig, l) - detr(ig, l) detr(ig, l) = 0. ! print*,'WARNING !!! detrainement negatif ',ig,l END IF END DO END DO ! RC IF (w2di==1) THEN fm0 = fm0 + ptimestep*(fm-fm0)/tho entr0 = entr0 + ptimestep*(entr-entr0)/tho ELSE fm0 = fm entr0 = entr END IF IF (1==1) THEN CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zh, zdhadj, & zha) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zo, pdoadj, & zoa) ELSE CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zh, & zdhadj, zha) CALL dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zo, & pdoadj, zoa) END IF IF (1==0) THEN CALL dvthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca, zmax, & zu, zv, pduadj, pdvadj, zua, zva) ELSE CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zu, pduadj, & zua) CALL dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse, zv, pdvadj, & zva) END IF DO l = 1, nlay DO ig = 1, ngrid zf = 0.5*(fracc(ig,l)+fracc(ig,l+1)) zf2 = zf/(1.-zf) thetath2(ig, l) = zf2*(zha(ig,l)-zh(ig,l))**2 wth2(ig, l) = zf2*(0.5*(wa_moy(ig,l)+wa_moy(ig,l+1)))**2 END DO END DO ! print*,'13 OK convect8' ! print*,'WA5 ',wa_moy DO l = 1, nlay DO ig = 1, ngrid pdtadj(ig, l) = zdhadj(ig, l)*zpspsk(ig, l) END DO END DO ! do l=1,nlay ! do ig=1,ngrid ! if(abs(pdtadj(ig,l))*86400..gt.500.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdtadj=',pdtadj(ig,l) ! endif ! if(abs(pdoadj(ig,l))*86400..gt.1.) then ! print*,'WARN!!! ig=',ig,' l=',l ! s ,' pdoadj=',pdoadj(ig,l) ! endif ! enddo ! enddo ! print*,'14 OK convect8' ! ------------------------------------------------------------------ ! Calculs pour les sorties ! ------------------------------------------------------------------ RETURN END SUBROUTINE thermcell_sec