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module thermcell_m |
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IMPLICIT NONE |
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contains |
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SUBROUTINE thermcell(ngrid, nlay, ptimestep, pplay, pplev, pphi, pu, pv, pt, & |
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po, pduadj, pdvadj, pdtadj, pdoadj, fm0, entr0, r_aspect, l_mix, w2di, & |
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tho) |
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! Calcul du transport vertical dans la couche limite en pr\'esence |
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! de "thermiques" explicitement repr\'esent\'es. R\'ecriture \`a partir |
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! d'un listing papier \`a Habas, le 14/02/00. Le thermique est |
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! suppos\'e homog\`ene et dissip\'e par m\'elange avec son |
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! environnement. La longueur "l_mix" contr\^ole l'efficacit\'e du |
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! m\'elange. Le calcul du transport des diff\'erentes esp\`eces se fait |
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! en prenant en compte : |
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! 1. un flux de masse montant |
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! 2. un flux de masse descendant |
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! 3. un entra\^inement |
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! 4. un d\'etra\^inement |
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USE dimphy, ONLY : klev, klon |
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USE suphec_m, ONLY : rd, rg, rkappa |
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! arguments: |
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INTEGER ngrid, nlay, w2di |
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real tho |
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real ptimestep, l_mix, r_aspect |
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REAL, intent(in):: pt(ngrid, nlay) |
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real pdtadj(ngrid, nlay) |
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REAL, intent(in):: pu(ngrid, nlay) |
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real pduadj(ngrid, nlay) |
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REAL, intent(in):: pv(ngrid, nlay) |
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real pdvadj(ngrid, nlay) |
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REAL po(ngrid, nlay), pdoadj(ngrid, nlay) |
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REAL, intent(in):: pplay(ngrid, nlay) |
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real, intent(in):: pplev(ngrid, nlay+1) |
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real, intent(in):: pphi(ngrid, nlay) |
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integer idetr |
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save idetr |
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data idetr/3/ |
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! local: |
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INTEGER ig, k, l, lmaxa(klon), lmix(klon) |
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! CR: on remplace lmax(klon, klev+1) |
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INTEGER lmax(klon), lmin(klon), lentr(klon) |
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real linter(klon) |
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real zmix(klon), fracazmix(klon) |
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real zmax(klon), zw, zw2(klon, klev+1), ztva(klon, klev) |
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real zlev(klon, klev+1) |
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REAL zh(klon, klev), zdhadj(klon, klev) |
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REAL ztv(klon, klev) |
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real zu(klon, klev), zv(klon, klev), zo(klon, klev) |
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real zva(klon, klev) |
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real zua(klon, klev) |
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real zoa(klon, klev) |
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real zha(klon, klev) |
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real wa_moy(klon, klev+1) |
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real fraca(klon, klev+1) |
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real fracc(klon, klev+1) |
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real zf, zf2 |
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real thetath2(klon, klev), wth2(klon, klev) |
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common/comtherm/thetath2, wth2 |
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real rho(klon, klev), rhobarz(klon, klev+1), masse(klon, klev) |
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real zpspsk(klon, klev) |
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real wmax(klon), wmaxa(klon) |
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real fracd(klon, klev+1) |
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real xxx(klon, klev+1) |
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real larg_cons(klon, klev+1) |
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real larg_detr(klon, klev+1) |
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real fm0(klon, klev+1), entr0(klon, klev), detr(klon, klev) |
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real fm(klon, klev+1), entr(klon, klev) |
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real fmc(klon, klev+1) |
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!CR:nouvelles variables |
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real f_star(klon, klev+1), entr_star(klon, klev) |
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real entr_star_tot(klon), entr_star2(klon) |
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real f(klon) |
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real zlevinter(klon) |
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EXTERNAL SCOPY |
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!----------------------------------------------------------------------- |
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! initialisation: |
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IF(ngrid.NE.klon) THEN |
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PRINT * |
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PRINT *, 'STOP dans convadj' |
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PRINT *, 'ngrid =', ngrid |
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PRINT *, 'klon =', klon |
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ENDIF |
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! incrementation eventuelle de tendances precedentes: |
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print *, '0 OK convect8' |
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DO l=1, nlay |
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DO ig=1, ngrid |
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zpspsk(ig, l)=(pplay(ig, l)/pplev(ig, 1))**RKAPPA |
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zh(ig, l)=pt(ig, l)/zpspsk(ig, l) |
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zu(ig, l)=pu(ig, l) |
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zv(ig, l)=pv(ig, l) |
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zo(ig, l)=po(ig, l) |
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ztv(ig, l)=zh(ig, l)*(1.+0.61*zo(ig, l)) |
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end DO |
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end DO |
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print *, '1 OK convect8' |
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! See notes, "thermcell.txt" |
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! Calcul des altitudes des couches |
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do l=2, nlay |
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do ig=1, ngrid |
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zlev(ig, l)=0.5*(pphi(ig, l)+pphi(ig, l-1))/RG |
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enddo |
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enddo |
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do ig=1, ngrid |
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zlev(ig, 1)=0. |
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zlev(ig, nlay+1)=(2.*pphi(ig, klev)-pphi(ig, klev-1))/RG |
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enddo |
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! Calcul des densites |
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do l=1, nlay |
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do ig=1, ngrid |
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rho(ig, l)=pplay(ig, l)/(zpspsk(ig, l)*RD*zh(ig, l)) |
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enddo |
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enddo |
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do l=2, nlay |
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do ig=1, ngrid |
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rhobarz(ig, l)=0.5*(rho(ig, l)+rho(ig, l-1)) |
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enddo |
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enddo |
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! Calcul de w2, quarre de w a partir de la cape |
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! a partir de w2, on calcule wa, vitesse de l'ascendance |
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! ATTENTION: Dans cette version, pour cause d'economie de memoire, |
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! w2 est stoke dans wa |
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! ATTENTION: dans convect8, on n'utilise le calcule des wa |
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! independants par couches que pour calculer l'entrainement |
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! a la base et la hauteur max de l'ascendance. |
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! Indicages: |
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! l'ascendance provenant du niveau k traverse l'interface l avec |
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! une vitesse wa(k, l). |
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! See notes, "thermcell.txt". |
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!CR: ponderation entrainement des couches instables |
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!def des entr_star tels que entr=f*entr_star |
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do l=1, klev |
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do ig=1, ngrid |
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entr_star(ig, l)=0. |
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enddo |
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enddo |
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! determination de la longueur de la couche d entrainement |
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do ig=1, ngrid |
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lentr(ig)=1 |
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enddo |
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!on ne considere que les premieres couches instables |
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do k=nlay-2, 1, -1 |
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do ig=1, ngrid |
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if (ztv(ig, k).gt.ztv(ig, k+1).and. & |
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ztv(ig, k+1).le.ztv(ig, k+2)) then |
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lentr(ig)=k |
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endif |
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enddo |
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enddo |
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! determination du lmin: couche d ou provient le thermique |
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do ig=1, ngrid |
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lmin(ig)=1 |
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enddo |
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do ig=1, ngrid |
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do l=nlay, 2, -1 |
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if (ztv(ig, l-1).gt.ztv(ig, l)) then |
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lmin(ig)=l-1 |
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endif |
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enddo |
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enddo |
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! definition de l'entrainement des couches |
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do l=1, klev-1 |
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do ig=1, ngrid |
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if (ztv(ig, l).gt.ztv(ig, l+1).and. & |
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l.ge.lmin(ig).and.l.le.lentr(ig)) then |
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entr_star(ig, l)=(ztv(ig, l)-ztv(ig, l+1))* & |
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(zlev(ig, l+1)-zlev(ig, l)) |
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endif |
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enddo |
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enddo |
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! pas de thermique si couches 1->5 stables |
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do ig=1, ngrid |
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if (lmin(ig).gt.5) then |
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do l=1, klev |
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entr_star(ig, l)=0. |
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enddo |
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endif |
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enddo |
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! calcul de l entrainement total |
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do ig=1, ngrid |
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entr_star_tot(ig)=0. |
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enddo |
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do ig=1, ngrid |
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do k=1, klev |
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entr_star_tot(ig)=entr_star_tot(ig)+entr_star(ig, k) |
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enddo |
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enddo |
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print *, 'fin calcul entr_star' |
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do k=1, klev |
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do ig=1, ngrid |
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ztva(ig, k)=ztv(ig, k) |
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enddo |
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enddo |
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do k=1, klev+1 |
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do ig=1, ngrid |
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zw2(ig, k)=0. |
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fmc(ig, k)=0. |
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f_star(ig, k)=0. |
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larg_cons(ig, k)=0. |
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larg_detr(ig, k)=0. |
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wa_moy(ig, k)=0. |
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enddo |
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enddo |
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do ig=1, ngrid |
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linter(ig)=1. |
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lmaxa(ig)=1 |
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lmix(ig)=1 |
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wmaxa(ig)=0. |
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enddo |
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do l=1, nlay-2 |
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do ig=1, ngrid |
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if (ztv(ig, l).gt.ztv(ig, l+1) & |
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.and.entr_star(ig, l).gt.1.e-10 & |
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.and.zw2(ig, l).lt.1e-10) then |
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f_star(ig, l+1)=entr_star(ig, l) |
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!test:calcul de dteta |
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zw2(ig, l+1)=2.*RG*(ztv(ig, l)-ztv(ig, l+1))/ztv(ig, l+1) & |
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*(zlev(ig, l+1)-zlev(ig, l)) & |
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*0.4*pphi(ig, l)/(pphi(ig, l+1)-pphi(ig, l)) |
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larg_detr(ig, l)=0. |
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else if ((zw2(ig, l).ge.1e-10).and. & |
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(f_star(ig, l)+entr_star(ig, l).gt.1.e-10)) then |
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f_star(ig, l+1)=f_star(ig, l)+entr_star(ig, l) |
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ztva(ig, l)=(f_star(ig, l)*ztva(ig, l-1)+entr_star(ig, l) & |
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*ztv(ig, l))/f_star(ig, l+1) |
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zw2(ig, l+1)=zw2(ig, l)*(f_star(ig, l)/f_star(ig, l+1))**2+ & |
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2.*RG*(ztva(ig, l)-ztv(ig, l))/ztv(ig, l) & |
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*(zlev(ig, l+1)-zlev(ig, l)) |
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endif |
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! determination de zmax continu par interpolation lineaire |
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if (zw2(ig, l+1).lt.0.) then |
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if (abs(zw2(ig, l+1)-zw2(ig, l)).lt.1e-10) then |
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print *, 'pb linter' |
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endif |
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linter(ig)=(l*(zw2(ig, l+1)-zw2(ig, l)) & |
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-zw2(ig, l))/(zw2(ig, l+1)-zw2(ig, l)) |
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zw2(ig, l+1)=0. |
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lmaxa(ig)=l |
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else |
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if (zw2(ig, l+1).lt.0.) then |
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print *, 'pb1 zw2<0' |
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endif |
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wa_moy(ig, l+1)=sqrt(zw2(ig, l+1)) |
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endif |
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if (wa_moy(ig, l+1).gt.wmaxa(ig)) then |
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! lmix est le niveau de la couche ou w (wa_moy) est maximum |
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lmix(ig)=l+1 |
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wmaxa(ig)=wa_moy(ig, l+1) |
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endif |
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enddo |
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enddo |
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print *, 'fin calcul zw2' |
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! Calcul de la couche correspondant a la hauteur du thermique |
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do ig=1, ngrid |
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lmax(ig)=lentr(ig) |
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enddo |
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do ig=1, ngrid |
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do l=nlay, lentr(ig)+1, -1 |
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if (zw2(ig, l).le.1.e-10) then |
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lmax(ig)=l-1 |
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endif |
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enddo |
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enddo |
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! pas de thermique si couches 1->5 stables |
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do ig=1, ngrid |
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if (lmin(ig).gt.5) then |
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lmax(ig)=1 |
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lmin(ig)=1 |
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endif |
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enddo |
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guez |
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! Determination de zw2 max |
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do ig=1, ngrid |
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wmax(ig)=0. |
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enddo |
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do l=1, nlay |
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do ig=1, ngrid |
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if (l.le.lmax(ig)) then |
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if (zw2(ig, l).lt.0.)then |
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print *, 'pb2 zw2<0' |
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endif |
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zw2(ig, l)=sqrt(zw2(ig, l)) |
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wmax(ig)=max(wmax(ig), zw2(ig, l)) |
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else |
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zw2(ig, l)=0. |
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endif |
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enddo |
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enddo |
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guez |
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guez |
54 |
! Longueur caracteristique correspondant a la hauteur des thermiques. |
| 334 |
|
|
do ig=1, ngrid |
| 335 |
|
|
zmax(ig)=0. |
| 336 |
|
|
zlevinter(ig)=zlev(ig, 1) |
| 337 |
|
|
enddo |
| 338 |
|
|
do ig=1, ngrid |
| 339 |
|
|
! calcul de zlevinter |
| 340 |
|
|
zlevinter(ig)=(zlev(ig, lmax(ig)+1)-zlev(ig, lmax(ig)))* & |
| 341 |
|
|
linter(ig)+zlev(ig, lmax(ig))-lmax(ig)*(zlev(ig, lmax(ig)+1) & |
| 342 |
|
|
-zlev(ig, lmax(ig))) |
| 343 |
|
|
zmax(ig)=max(zmax(ig), zlevinter(ig)-zlev(ig, lmin(ig))) |
| 344 |
|
|
enddo |
| 345 |
guez |
3 |
|
| 346 |
guez |
54 |
print *, 'avant fermeture' |
| 347 |
|
|
! Fermeture, determination de f |
| 348 |
|
|
do ig=1, ngrid |
| 349 |
|
|
entr_star2(ig)=0. |
| 350 |
|
|
enddo |
| 351 |
|
|
do ig=1, ngrid |
| 352 |
|
|
if (entr_star_tot(ig).LT.1.e-10) then |
| 353 |
|
|
f(ig)=0. |
| 354 |
|
|
else |
| 355 |
|
|
do k=lmin(ig), lentr(ig) |
| 356 |
|
|
entr_star2(ig)=entr_star2(ig)+entr_star(ig, k)**2 & |
| 357 |
|
|
/(rho(ig, k)*(zlev(ig, k+1)-zlev(ig, k))) |
| 358 |
|
|
enddo |
| 359 |
|
|
! Nouvelle fermeture |
| 360 |
|
|
f(ig)=wmax(ig)/(max(500., zmax(ig))*r_aspect & |
| 361 |
|
|
*entr_star2(ig))*entr_star_tot(ig) |
| 362 |
|
|
endif |
| 363 |
|
|
enddo |
| 364 |
|
|
print *, 'apres fermeture' |
| 365 |
guez |
3 |
|
| 366 |
guez |
54 |
! Calcul de l'entrainement |
| 367 |
|
|
do k=1, klev |
| 368 |
|
|
do ig=1, ngrid |
| 369 |
|
|
entr(ig, k)=f(ig)*entr_star(ig, k) |
| 370 |
|
|
enddo |
| 371 |
|
|
enddo |
| 372 |
|
|
! Calcul des flux |
| 373 |
|
|
do ig=1, ngrid |
| 374 |
|
|
do l=1, lmax(ig)-1 |
| 375 |
|
|
fmc(ig, l+1)=fmc(ig, l)+entr(ig, l) |
| 376 |
|
|
enddo |
| 377 |
|
|
enddo |
| 378 |
guez |
3 |
|
| 379 |
guez |
54 |
! determination de l'indice du debut de la mixed layer ou w decroit |
| 380 |
guez |
3 |
|
| 381 |
guez |
54 |
! calcul de la largeur de chaque ascendance dans le cas conservatif. |
| 382 |
|
|
! dans ce cas simple, on suppose que la largeur de l'ascendance provenant |
| 383 |
guez |
150 |
! d'une couche est \'egale \`a la hauteur de la couche alimentante. |
| 384 |
guez |
54 |
! La vitesse maximale dans l'ascendance est aussi prise comme estimation |
| 385 |
|
|
! de la vitesse d'entrainement horizontal dans la couche alimentante. |
| 386 |
guez |
3 |
|
| 387 |
guez |
54 |
do l=2, nlay |
| 388 |
|
|
do ig=1, ngrid |
| 389 |
|
|
if (l.le.lmaxa(ig)) then |
| 390 |
|
|
zw=max(wa_moy(ig, l), 1.e-10) |
| 391 |
|
|
larg_cons(ig, l)=zmax(ig)*r_aspect & |
| 392 |
|
|
*fmc(ig, l)/(rhobarz(ig, l)*zw) |
| 393 |
|
|
endif |
| 394 |
|
|
enddo |
| 395 |
|
|
enddo |
| 396 |
guez |
3 |
|
| 397 |
guez |
54 |
do l=2, nlay |
| 398 |
|
|
do ig=1, ngrid |
| 399 |
|
|
if (l.le.lmaxa(ig)) then |
| 400 |
|
|
if ((l_mix*zlev(ig, l)).lt.0.)then |
| 401 |
|
|
print *, 'pb l_mix*zlev<0' |
| 402 |
|
|
endif |
| 403 |
|
|
larg_detr(ig, l)=sqrt(l_mix*zlev(ig, l)) |
| 404 |
|
|
endif |
| 405 |
|
|
enddo |
| 406 |
|
|
enddo |
| 407 |
guez |
3 |
|
| 408 |
guez |
150 |
! calcul de la fraction de la maille concern\'ee par l'ascendance en tenant |
| 409 |
guez |
54 |
! compte de l'epluchage du thermique. |
| 410 |
guez |
3 |
|
| 411 |
guez |
54 |
!CR def de zmix continu (profil parabolique des vitesses) |
| 412 |
|
|
do ig=1, ngrid |
| 413 |
|
|
if (lmix(ig).gt.1.) then |
| 414 |
|
|
if (((zw2(ig, lmix(ig)-1)-zw2(ig, lmix(ig))) & |
| 415 |
|
|
*((zlev(ig, lmix(ig)))-(zlev(ig, lmix(ig)+1))) & |
| 416 |
|
|
-(zw2(ig, lmix(ig))-zw2(ig, lmix(ig)+1)) & |
| 417 |
|
|
*((zlev(ig, lmix(ig)-1))-(zlev(ig, lmix(ig))))).gt.1e-10) & |
| 418 |
|
|
then |
| 419 |
guez |
3 |
|
| 420 |
guez |
54 |
zmix(ig)=((zw2(ig, lmix(ig)-1)-zw2(ig, lmix(ig))) & |
| 421 |
|
|
*((zlev(ig, lmix(ig)))**2-(zlev(ig, lmix(ig)+1))**2) & |
| 422 |
|
|
-(zw2(ig, lmix(ig))-zw2(ig, lmix(ig)+1)) & |
| 423 |
|
|
*((zlev(ig, lmix(ig)-1))**2-(zlev(ig, lmix(ig)))**2)) & |
| 424 |
|
|
/(2.*((zw2(ig, lmix(ig)-1)-zw2(ig, lmix(ig))) & |
| 425 |
|
|
*((zlev(ig, lmix(ig)))-(zlev(ig, lmix(ig)+1))) & |
| 426 |
|
|
-(zw2(ig, lmix(ig))-zw2(ig, lmix(ig)+1)) & |
| 427 |
|
|
*((zlev(ig, lmix(ig)-1))-(zlev(ig, lmix(ig)))))) |
| 428 |
|
|
else |
| 429 |
|
|
zmix(ig)=zlev(ig, lmix(ig)) |
| 430 |
|
|
print *, 'pb zmix' |
| 431 |
|
|
endif |
| 432 |
|
|
else |
| 433 |
|
|
zmix(ig)=0. |
| 434 |
|
|
endif |
| 435 |
guez |
3 |
|
| 436 |
guez |
54 |
if ((zmax(ig)-zmix(ig)).lt.0.) then |
| 437 |
|
|
zmix(ig)=0.99*zmax(ig) |
| 438 |
|
|
endif |
| 439 |
|
|
enddo |
| 440 |
guez |
3 |
|
| 441 |
guez |
54 |
! calcul du nouveau lmix correspondant |
| 442 |
|
|
do ig=1, ngrid |
| 443 |
|
|
do l=1, klev |
| 444 |
|
|
if (zmix(ig).ge.zlev(ig, l).and. & |
| 445 |
|
|
zmix(ig).lt.zlev(ig, l+1)) then |
| 446 |
|
|
lmix(ig)=l |
| 447 |
|
|
endif |
| 448 |
|
|
enddo |
| 449 |
|
|
enddo |
| 450 |
guez |
3 |
|
| 451 |
guez |
54 |
do l=2, nlay |
| 452 |
|
|
do ig=1, ngrid |
| 453 |
|
|
if(larg_cons(ig, l).gt.1.) then |
| 454 |
|
|
fraca(ig, l)=(larg_cons(ig, l)-larg_detr(ig, l)) & |
| 455 |
|
|
/(r_aspect*zmax(ig)) |
| 456 |
|
|
fraca(ig, l)=max(fraca(ig, l), 0.) |
| 457 |
|
|
fraca(ig, l)=min(fraca(ig, l), 0.5) |
| 458 |
|
|
fracd(ig, l)=1.-fraca(ig, l) |
| 459 |
|
|
fracc(ig, l)=larg_cons(ig, l)/(r_aspect*zmax(ig)) |
| 460 |
|
|
else |
| 461 |
|
|
fraca(ig, l)=0. |
| 462 |
|
|
fracc(ig, l)=0. |
| 463 |
|
|
fracd(ig, l)=1. |
| 464 |
|
|
endif |
| 465 |
|
|
enddo |
| 466 |
|
|
enddo |
| 467 |
|
|
!CR: calcul de fracazmix |
| 468 |
|
|
do ig=1, ngrid |
| 469 |
|
|
fracazmix(ig)=(fraca(ig, lmix(ig)+1)-fraca(ig, lmix(ig)))/ & |
| 470 |
|
|
(zlev(ig, lmix(ig)+1)-zlev(ig, lmix(ig)))*zmix(ig) & |
| 471 |
|
|
+fraca(ig, lmix(ig))-zlev(ig, lmix(ig))*(fraca(ig, lmix(ig)+1) & |
| 472 |
|
|
-fraca(ig, lmix(ig)))/(zlev(ig, lmix(ig)+1)-zlev(ig, lmix(ig))) |
| 473 |
|
|
enddo |
| 474 |
guez |
3 |
|
| 475 |
guez |
54 |
do l=2, nlay |
| 476 |
|
|
do ig=1, ngrid |
| 477 |
|
|
if(larg_cons(ig, l).gt.1.) then |
| 478 |
|
|
if (l.gt.lmix(ig)) then |
| 479 |
|
|
if (zmax(ig)-zmix(ig).lt.1.e-10) then |
| 480 |
|
|
xxx(ig, l)=(lmaxa(ig)+1.-l)/(lmaxa(ig)+1.-lmix(ig)) |
| 481 |
|
|
else |
| 482 |
|
|
xxx(ig, l)=(zmax(ig)-zlev(ig, l))/(zmax(ig)-zmix(ig)) |
| 483 |
|
|
endif |
| 484 |
|
|
if (idetr.eq.0) then |
| 485 |
|
|
fraca(ig, l)=fracazmix(ig) |
| 486 |
|
|
else if (idetr.eq.1) then |
| 487 |
|
|
fraca(ig, l)=fracazmix(ig)*xxx(ig, l) |
| 488 |
|
|
else if (idetr.eq.2) then |
| 489 |
|
|
fraca(ig, l)=fracazmix(ig)*(1.-(1.-xxx(ig, l))**2) |
| 490 |
|
|
else |
| 491 |
|
|
fraca(ig, l)=fracazmix(ig)*xxx(ig, l)**2 |
| 492 |
|
|
endif |
| 493 |
|
|
fraca(ig, l)=max(fraca(ig, l), 0.) |
| 494 |
|
|
fraca(ig, l)=min(fraca(ig, l), 0.5) |
| 495 |
|
|
fracd(ig, l)=1.-fraca(ig, l) |
| 496 |
|
|
fracc(ig, l)=larg_cons(ig, l)/(r_aspect*zmax(ig)) |
| 497 |
|
|
endif |
| 498 |
|
|
endif |
| 499 |
|
|
enddo |
| 500 |
|
|
enddo |
| 501 |
guez |
3 |
|
| 502 |
guez |
54 |
print *, 'fin calcul fraca' |
| 503 |
guez |
3 |
|
| 504 |
guez |
54 |
! Calcul de fracd, wd |
| 505 |
|
|
! somme wa - wd = 0 |
| 506 |
guez |
3 |
|
| 507 |
guez |
54 |
do ig=1, ngrid |
| 508 |
|
|
fm(ig, 1)=0. |
| 509 |
|
|
fm(ig, nlay+1)=0. |
| 510 |
|
|
enddo |
| 511 |
guez |
3 |
|
| 512 |
guez |
54 |
do l=2, nlay |
| 513 |
|
|
do ig=1, ngrid |
| 514 |
|
|
fm(ig, l)=fraca(ig, l)*wa_moy(ig, l)*rhobarz(ig, l) |
| 515 |
|
|
if (entr(ig, l-1).lt.1e-10.and.fm(ig, l).gt.fm(ig, l-1) & |
| 516 |
|
|
.and.l.gt.lmix(ig)) then |
| 517 |
|
|
fm(ig, l)=fm(ig, l-1) |
| 518 |
|
|
endif |
| 519 |
|
|
enddo |
| 520 |
|
|
do ig=1, ngrid |
| 521 |
|
|
if(fracd(ig, l).lt.0.1) then |
| 522 |
|
|
stop'fracd trop petit' |
| 523 |
|
|
endif |
| 524 |
|
|
enddo |
| 525 |
|
|
enddo |
| 526 |
guez |
3 |
|
| 527 |
guez |
54 |
do l=1, nlay |
| 528 |
|
|
do ig=1, ngrid |
| 529 |
|
|
masse(ig, l)=(pplev(ig, l)-pplev(ig, l+1))/RG |
| 530 |
|
|
enddo |
| 531 |
|
|
enddo |
| 532 |
guez |
3 |
|
| 533 |
guez |
54 |
print *, '12 OK convect8' |
| 534 |
guez |
3 |
|
| 535 |
guez |
54 |
! calcul du transport vertical |
| 536 |
guez |
3 |
|
| 537 |
guez |
54 |
!CR:redefinition du entr |
| 538 |
|
|
do l=1, nlay |
| 539 |
|
|
do ig=1, ngrid |
| 540 |
|
|
detr(ig, l)=fm(ig, l)+entr(ig, l)-fm(ig, l+1) |
| 541 |
|
|
if (detr(ig, l).lt.0.) then |
| 542 |
|
|
entr(ig, l)=entr(ig, l)-detr(ig, l) |
| 543 |
|
|
detr(ig, l)=0. |
| 544 |
|
|
endif |
| 545 |
|
|
enddo |
| 546 |
|
|
enddo |
| 547 |
guez |
3 |
|
| 548 |
guez |
54 |
if (w2di.eq.1) then |
| 549 |
|
|
fm0=fm0+ptimestep*(fm-fm0)/tho |
| 550 |
|
|
entr0=entr0+ptimestep*(entr-entr0)/tho |
| 551 |
|
|
else |
| 552 |
|
|
fm0=fm |
| 553 |
|
|
entr0=entr |
| 554 |
|
|
endif |
| 555 |
guez |
3 |
|
| 556 |
guez |
54 |
if (1.eq.1) then |
| 557 |
|
|
call dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse & |
| 558 |
|
|
, zh, zdhadj, zha) |
| 559 |
|
|
call dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse & |
| 560 |
|
|
, zo, pdoadj, zoa) |
| 561 |
|
|
else |
| 562 |
|
|
call dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca & |
| 563 |
|
|
, zh, zdhadj, zha) |
| 564 |
|
|
call dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca & |
| 565 |
|
|
, zo, pdoadj, zoa) |
| 566 |
|
|
endif |
| 567 |
guez |
3 |
|
| 568 |
guez |
54 |
if (1.eq.0) then |
| 569 |
|
|
call dvthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse & |
| 570 |
|
|
, fraca, zmax & |
| 571 |
|
|
, zu, zv, pduadj, pdvadj, zua, zva) |
| 572 |
|
|
else |
| 573 |
|
|
call dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse & |
| 574 |
|
|
, zu, pduadj, zua) |
| 575 |
|
|
call dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse & |
| 576 |
|
|
, zv, pdvadj, zva) |
| 577 |
|
|
endif |
| 578 |
guez |
3 |
|
| 579 |
guez |
54 |
do l=1, nlay |
| 580 |
|
|
do ig=1, ngrid |
| 581 |
|
|
zf=0.5*(fracc(ig, l)+fracc(ig, l+1)) |
| 582 |
|
|
zf2=zf/(1.-zf) |
| 583 |
|
|
thetath2(ig, l)=zf2*(zha(ig, l)-zh(ig, l))**2 |
| 584 |
|
|
wth2(ig, l)=zf2*(0.5*(wa_moy(ig, l)+wa_moy(ig, l+1)))**2 |
| 585 |
|
|
enddo |
| 586 |
|
|
enddo |
| 587 |
guez |
3 |
|
| 588 |
guez |
54 |
do l=1, nlay |
| 589 |
|
|
do ig=1, ngrid |
| 590 |
|
|
pdtadj(ig, l)=zdhadj(ig, l)*zpspsk(ig, l) |
| 591 |
|
|
enddo |
| 592 |
|
|
enddo |
| 593 |
guez |
3 |
|
| 594 |
guez |
54 |
end SUBROUTINE thermcell |
| 595 |
guez |
3 |
|
| 596 |
guez |
54 |
end module thermcell_m |
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