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module phystokenc_m |
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! $Header: /home/cvsroot/LMDZ4/libf/phylmd/phystokenc.F,v 1.2 2004/06/22 11:45:35 lmdzadmin Exp $ |
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! |
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c |
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c |
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SUBROUTINE phystokenc ( |
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I pdtphys,rlon,rlat, |
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I pt,pmfu, pmfd, pen_u, pde_u, pen_d, pde_d, |
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I pfm_therm,pentr_therm, |
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I pcoefh,yu1,yv1,ftsol,pctsrf, |
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I frac_impa,frac_nucl, |
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I pphis,paire,dtime,itap) |
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USE ioipsl |
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USE histcom |
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use dimens_m |
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use indicesol |
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use dimphy |
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use conf_gcm_m |
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use tracstoke |
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IMPLICIT none |
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c====================================================================== |
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c Auteur(s) FH |
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c Objet: Moniteur general des tendances traceurs |
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c |
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c====================================================================== |
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c====================================================================== |
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c Arguments: |
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c |
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c EN ENTREE: |
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c ========== |
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c |
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c divers: |
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c ------- |
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c |
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real pdtphys ! pas d'integration pour la physique (seconde) |
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c |
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integer physid, itap |
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save physid |
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integer ndex2d(iim*(jjm+1)),ndex3d(iim*(jjm+1)*klev) |
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c convection: |
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c ----------- |
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c |
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REAL pmfu(klon,klev) ! flux de masse dans le panache montant |
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REAL pmfd(klon,klev) ! flux de masse dans le panache descendant |
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REAL pen_u(klon,klev) ! flux entraine dans le panache montant |
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REAL pde_u(klon,klev) ! flux detraine dans le panache montant |
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REAL pen_d(klon,klev) ! flux entraine dans le panache descendant |
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REAL pde_d(klon,klev) ! flux detraine dans le panache descendant |
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real pt(klon,klev),t(klon,klev) |
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c |
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REAL, intent(in):: rlon(klon), rlat(klon) |
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real dtime |
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REAL zx_tmp_3d(iim,jjm+1,klev),zx_tmp_2d(iim,jjm+1) |
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c Couche limite: |
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c -------------- |
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c |
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REAL pcoefh(klon,klev) ! coeff melange CL |
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REAL yv1(klon) |
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REAL yu1(klon),pphis(klon),paire(klon) |
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c Les Thermiques : (Abderr 25 11 02) |
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c --------------- |
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REAL pfm_therm(klon,klev+1) |
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real fm_therm1(klon,klev) |
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REAL pentr_therm(klon,klev) |
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REAL entr_therm(klon,klev) |
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REAL fm_therm(klon,klev) |
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c |
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c Lessivage: |
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c ---------- |
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c |
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REAL frac_impa(klon,klev) |
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REAL frac_nucl(klon,klev) |
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c |
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c Arguments necessaires pour les sources et puits de traceur |
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C |
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real ftsol(klon,nbsrf) ! Temperature du sol (surf)(Kelvin) |
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real pctsrf(klon,nbsrf) ! Pourcentage de sol f(nature du sol) |
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c====================================================================== |
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c |
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INTEGER i, k |
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c |
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REAL mfu(klon,klev) ! flux de masse dans le panache montant |
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REAL mfd(klon,klev) ! flux de masse dans le panache descendant |
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REAL en_u(klon,klev) ! flux entraine dans le panache montant |
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REAL de_u(klon,klev) ! flux detraine dans le panache montant |
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REAL en_d(klon,klev) ! flux entraine dans le panache descendant |
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REAL de_d(klon,klev) ! flux detraine dans le panache descendant |
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REAL coefh(klon,klev) ! flux detraine dans le panache descendant |
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REAL pyu1(klon),pyv1(klon) |
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REAL pftsol(klon,nbsrf),ppsrf(klon,nbsrf) |
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real pftsol1(klon),pftsol2(klon),pftsol3(klon),pftsol4(klon) |
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real ppsrf1(klon),ppsrf2(klon),ppsrf3(klon),ppsrf4(klon) |
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REAL dtcum |
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integer iadvtr,irec |
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real zmin,zmax |
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logical ok_sync |
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save t,mfu,mfd,en_u,de_u,en_d,de_d,coefh,dtcum |
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save fm_therm,entr_therm |
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save iadvtr,irec |
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save pyu1,pyv1,pftsol,ppsrf |
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data iadvtr,irec/0,1/ |
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c |
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c Couche limite: |
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c====================================================================== |
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ok_sync = .true. |
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print*,'Dans phystokenc.F' |
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print*,'iadvtr= ',iadvtr |
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print*,'istphy= ',istphy |
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print*,'istdyn= ',istdyn |
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IF (iadvtr.eq.0) THEN |
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CALL initphysto('phystoke', |
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. rlon,rlat,dtime, dtime*istphy,dtime*istphy,nqmx,physid) |
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write(*,*) 'apres initphysto ds phystokenc' |
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ENDIF |
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c |
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ndex2d = 0 |
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ndex3d = 0 |
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i=itap |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1,pphis,zx_tmp_2d) |
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CALL histwrite(physid,"phis",i,zx_tmp_2d,iim*(jjm+1),ndex2d) |
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c |
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i=itap |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1,paire,zx_tmp_2d) |
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CALL histwrite(physid,"aire",i,zx_tmp_2d,iim*(jjm+1),ndex2d) |
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iadvtr=iadvtr+1 |
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c |
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if (mod(iadvtr,istphy).eq.1.or.istphy.eq.1) then |
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print*,'reinitialisation des champs cumules |
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s a iadvtr=',iadvtr |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=0. |
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mfd(i,k)=0. |
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en_u(i,k)=0. |
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de_u(i,k)=0. |
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en_d(i,k)=0. |
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de_d(i,k)=0. |
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coefh(i,k)=0. |
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t(i,k)=0. |
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fm_therm(i,k)=0. |
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entr_therm(i,k)=0. |
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enddo |
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enddo |
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do i=1,klon |
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pyv1(i)=0. |
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pyu1(i)=0. |
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end do |
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do k=1,nbsrf |
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do i=1,klon |
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pftsol(i,k)=0. |
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ppsrf(i,k)=0. |
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enddo |
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enddo |
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dtcum=0. |
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endif |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=mfu(i,k)+pmfu(i,k)*pdtphys |
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mfd(i,k)=mfd(i,k)+pmfd(i,k)*pdtphys |
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en_u(i,k)=en_u(i,k)+pen_u(i,k)*pdtphys |
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de_u(i,k)=de_u(i,k)+pde_u(i,k)*pdtphys |
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en_d(i,k)=en_d(i,k)+pen_d(i,k)*pdtphys |
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de_d(i,k)=de_d(i,k)+pde_d(i,k)*pdtphys |
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coefh(i,k)=coefh(i,k)+pcoefh(i,k)*pdtphys |
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t(i,k)=t(i,k)+pt(i,k)*pdtphys |
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fm_therm(i,k)=fm_therm(i,k)+pfm_therm(i,k)*pdtphys |
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entr_therm(i,k)=entr_therm(i,k)+pentr_therm(i,k)*pdtphys |
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enddo |
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enddo |
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do i=1,klon |
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pyv1(i)=pyv1(i)+yv1(i)*pdtphys |
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pyu1(i)=pyu1(i)+yu1(i)*pdtphys |
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end do |
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do k=1,nbsrf |
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do i=1,klon |
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pftsol(i,k)=pftsol(i,k)+ftsol(i,k)*pdtphys |
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ppsrf(i,k)=ppsrf(i,k)+pctsrf(i,k)*pdtphys |
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enddo |
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enddo |
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dtcum=dtcum+pdtphys |
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IF(mod(iadvtr,istphy).eq.0) THEN |
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c |
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c normalisation par le temps cumule |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=mfu(i,k)/dtcum |
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mfd(i,k)=mfd(i,k)/dtcum |
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en_u(i,k)=en_u(i,k)/dtcum |
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de_u(i,k)=de_u(i,k)/dtcum |
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en_d(i,k)=en_d(i,k)/dtcum |
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de_d(i,k)=de_d(i,k)/dtcum |
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coefh(i,k)=coefh(i,k)/dtcum |
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c Unitel a enlever |
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t(i,k)=t(i,k)/dtcum |
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fm_therm(i,k)=fm_therm(i,k)/dtcum |
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entr_therm(i,k)=entr_therm(i,k)/dtcum |
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enddo |
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enddo |
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do i=1,klon |
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pyv1(i)=pyv1(i)/dtcum |
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pyu1(i)=pyu1(i)/dtcum |
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end do |
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do k=1,nbsrf |
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do i=1,klon |
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pftsol(i,k)=pftsol(i,k)/dtcum |
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pftsol1(i) = pftsol(i,1) |
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pftsol2(i) = pftsol(i,2) |
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pftsol3(i) = pftsol(i,3) |
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pftsol4(i) = pftsol(i,4) |
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ppsrf(i,k)=ppsrf(i,k)/dtcum |
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ppsrf1(i) = ppsrf(i,1) |
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ppsrf2(i) = ppsrf(i,2) |
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ppsrf3(i) = ppsrf(i,3) |
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ppsrf4(i) = ppsrf(i,4) |
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enddo |
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enddo |
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c |
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c ecriture des champs |
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c |
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irec=irec+1 |
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ccccc |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, t, zx_tmp_3d) |
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CALL histwrite(physid,"t",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, mfu, zx_tmp_3d) |
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CALL histwrite(physid,"mfu",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, mfd, zx_tmp_3d) |
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CALL histwrite(physid,"mfd",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, en_u, zx_tmp_3d) |
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CALL histwrite(physid,"en_u",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, de_u, zx_tmp_3d) |
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CALL histwrite(physid,"de_u",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, en_d, zx_tmp_3d) |
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CALL histwrite(physid,"en_d",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, de_d, zx_tmp_3d) |
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CALL histwrite(physid,"de_d",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, coefh, zx_tmp_3d) |
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CALL histwrite(physid,"coefh",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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c ajou... |
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do k=1,klev |
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do i=1,klon |
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fm_therm1(i,k)=fm_therm(i,k) |
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enddo |
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enddo |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, fm_therm1, zx_tmp_3d) |
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CALL histwrite(physid,"fm_th",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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c |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, entr_therm, zx_tmp_3d) |
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CALL histwrite(physid,"en_th",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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cccc |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1,frac_impa,zx_tmp_3d) |
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CALL histwrite(physid,"frac_impa",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1,frac_nucl,zx_tmp_3d) |
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CALL histwrite(physid,"frac_nucl",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(1, klon,iim,jjm+1, pyu1,zx_tmp_2d) |
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CALL histwrite(physid,"pyu1",itap,zx_tmp_2d,iim*(jjm+1), |
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. ndex2d) |
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CALL gr_fi_ecrit(1, klon,iim,jjm+1, pyv1,zx_tmp_2d) |
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CALL histwrite(physid,"pyv1",itap,zx_tmp_2d,iim*(jjm+1) |
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. ,ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol1, zx_tmp_2d) |
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CALL histwrite(physid,"ftsol1",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol2, zx_tmp_2d) |
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CALL histwrite(physid,"ftsol2",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol3, zx_tmp_2d) |
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CALL histwrite(physid,"ftsol3",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol4, zx_tmp_2d) |
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CALL histwrite(physid,"ftsol4",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf1, zx_tmp_2d) |
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CALL histwrite(physid,"psrf1",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf2, zx_tmp_2d) |
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CALL histwrite(physid,"psrf2",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf3, zx_tmp_2d) |
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CALL histwrite(physid,"psrf3",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf4, zx_tmp_2d) |
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CALL histwrite(physid,"psrf4",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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if (ok_sync) call histsync(physid) |
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c if (ok_sync) call histsync |
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c |
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cAA Test sur la valeur des coefficients de lessivage |
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c |
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zmin=1e33 |
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zmax=-1e33 |
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do k=1,klev |
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do i=1,klon |
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zmax=max(zmax,frac_nucl(i,k)) |
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zmin=min(zmin,frac_nucl(i,k)) |
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enddo |
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enddo |
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Print*,'------ coefs de lessivage (min et max) --------' |
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Print*,'facteur de nucleation ',zmin,zmax |
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zmin=1e33 |
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zmax=-1e33 |
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do k=1,klev |
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do i=1,klon |
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zmax=max(zmax,frac_impa(i,k)) |
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zmin=min(zmin,frac_impa(i,k)) |
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enddo |
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enddo |
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Print*,'facteur d impaction ',zmin,zmax |
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ENDIF |
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c reinitialisation des champs cumules |
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go to 768 |
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if (mod(iadvtr,istphy).eq.1) then |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=0. |
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mfd(i,k)=0. |
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en_u(i,k)=0. |
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de_u(i,k)=0. |
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en_d(i,k)=0. |
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de_d(i,k)=0. |
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coefh(i,k)=0. |
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t(i,k)=0. |
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fm_therm(i,k)=0. |
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entr_therm(i,k)=0. |
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enddo |
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enddo |
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do i=1,klon |
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pyv1(i)=0. |
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pyu1(i)=0. |
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end do |
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do k=1,nbsrf |
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do i=1,klon |
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pftsol(i,k)=0. |
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ppsrf(i,k)=0. |
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enddo |
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enddo |
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dtcum=0. |
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endif |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=mfu(i,k)+pmfu(i,k)*pdtphys |
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mfd(i,k)=mfd(i,k)+pmfd(i,k)*pdtphys |
|
|
en_u(i,k)=en_u(i,k)+pen_u(i,k)*pdtphys |
|
|
de_u(i,k)=de_u(i,k)+pde_u(i,k)*pdtphys |
|
|
en_d(i,k)=en_d(i,k)+pen_d(i,k)*pdtphys |
|
|
de_d(i,k)=de_d(i,k)+pde_d(i,k)*pdtphys |
|
|
coefh(i,k)=coefh(i,k)+pcoefh(i,k)*pdtphys |
|
|
t(i,k)=t(i,k)+pt(i,k)*pdtphys |
|
|
fm_therm(i,k)=fm_therm(i,k)+pfm_therm(i,k)*pdtphys |
|
|
entr_therm(i,k)=entr_therm(i,k)+pentr_therm(i,k)*pdtphys |
|
|
enddo |
|
|
enddo |
|
|
do i=1,klon |
|
|
pyv1(i)=pyv1(i)+yv1(i)*pdtphys |
|
|
pyu1(i)=pyu1(i)+yu1(i)*pdtphys |
|
|
end do |
|
|
do k=1,nbsrf |
|
|
do i=1,klon |
|
|
pftsol(i,k)=pftsol(i,k)+ftsol(i,k)*pdtphys |
|
|
ppsrf(i,k)=ppsrf(i,k)+pctsrf(i,k)*pdtphys |
|
|
enddo |
|
|
enddo |
|
| 2 |
|
|
| 3 |
dtcum=dtcum+pdtphys |
IMPLICIT NONE |
|
768 continue |
|
| 4 |
|
|
| 5 |
RETURN |
contains |
| 6 |
END |
|
| 7 |
|
SUBROUTINE phystokenc(pdtphys, rlon, rlat, pt, pmfu, pmfd, pen_u, pde_u, & |
| 8 |
|
pen_d, pde_d, pfm_therm, pentr_therm, pcoefh, yu1, yv1, ftsol, pctsrf, & |
| 9 |
|
frac_impa, frac_nucl, pphis, paire, dtime, itap) |
| 10 |
|
|
| 11 |
|
! From phylmd/phystokenc.F, version 1.2 2004/06/22 11:45:35 |
| 12 |
|
! Author: Fr\'ed\'eric Hourdin |
| 13 |
|
! Objet : \'ecriture des variables pour transport offline |
| 14 |
|
|
| 15 |
|
use gr_phy_write_m, only: gr_phy_write |
| 16 |
|
USE histwrite_m, ONLY: histwrite |
| 17 |
|
USE histsync_m, ONLY: histsync |
| 18 |
|
USE dimens_m, ONLY: iim, jjm |
| 19 |
|
USE indicesol, ONLY: nbsrf |
| 20 |
|
use initphysto_m, only: initphysto |
| 21 |
|
USE dimphy, ONLY: klev, klon |
| 22 |
|
USE tracstoke, ONLY: istphy |
| 23 |
|
|
| 24 |
|
REAL, INTENT (IN):: pdtphys ! pas d'integration pour la physique (seconde) |
| 25 |
|
REAL, INTENT (IN):: rlon(klon), rlat(klon) |
| 26 |
|
REAL, intent(in):: pt(klon, klev) |
| 27 |
|
|
| 28 |
|
! convection: |
| 29 |
|
|
| 30 |
|
REAL, INTENT (IN):: pmfu(klon, klev) ! flux de masse dans le panache montant |
| 31 |
|
|
| 32 |
|
REAL, intent(in):: pmfd(klon, klev) |
| 33 |
|
! flux de masse dans le panache descendant |
| 34 |
|
|
| 35 |
|
REAL, intent(in):: pen_u(klon, klev) ! flux entraine dans le panache montant |
| 36 |
|
REAL, intent(in):: pde_u(klon, klev) ! flux detraine dans le panache montant |
| 37 |
|
|
| 38 |
|
REAL, intent(in):: pen_d(klon, klev) |
| 39 |
|
! flux entraine dans le panache descendant |
| 40 |
|
|
| 41 |
|
REAL, intent(in):: pde_d(klon, klev) |
| 42 |
|
! flux detraine dans le panache descendant |
| 43 |
|
|
| 44 |
|
! Les Thermiques |
| 45 |
|
REAL pfm_therm(klon, klev+1) |
| 46 |
|
REAL pentr_therm(klon, klev) |
| 47 |
|
|
| 48 |
|
! Couche limite: |
| 49 |
|
|
| 50 |
|
REAL pcoefh(klon, klev) ! coeff melange Couche limite |
| 51 |
|
REAL yu1(klon) |
| 52 |
|
REAL yv1(klon) |
| 53 |
|
|
| 54 |
|
! Arguments necessaires pour les sources et puits de traceur |
| 55 |
|
|
| 56 |
|
REAL ftsol(klon, nbsrf) ! Temperature du sol (surf)(Kelvin) |
| 57 |
|
REAL pctsrf(klon, nbsrf) ! Pourcentage de sol f(nature du sol) |
| 58 |
|
|
| 59 |
|
! Lessivage: |
| 60 |
|
|
| 61 |
|
REAL frac_impa(klon, klev) |
| 62 |
|
REAL frac_nucl(klon, klev) |
| 63 |
|
|
| 64 |
|
REAL, INTENT(IN):: pphis(klon) |
| 65 |
|
real paire(klon) |
| 66 |
|
REAL, INTENT (IN):: dtime |
| 67 |
|
INTEGER, INTENT (IN):: itap |
| 68 |
|
|
| 69 |
|
! Variables local to the procedure: |
| 70 |
|
|
| 71 |
|
real t(klon, klev) |
| 72 |
|
INTEGER, SAVE:: physid |
| 73 |
|
REAL zx_tmp_3d(iim, jjm+1, klev), zx_tmp_2d(iim, jjm+1) |
| 74 |
|
|
| 75 |
|
! Les Thermiques |
| 76 |
|
|
| 77 |
|
REAL fm_therm1(klon, klev) |
| 78 |
|
REAL entr_therm(klon, klev) |
| 79 |
|
REAL fm_therm(klon, klev) |
| 80 |
|
|
| 81 |
|
INTEGER i, k |
| 82 |
|
|
| 83 |
|
REAL, save:: mfu(klon, klev) ! flux de masse dans le panache montant |
| 84 |
|
REAL mfd(klon, klev) ! flux de masse dans le panache descendant |
| 85 |
|
REAL en_u(klon, klev) ! flux entraine dans le panache montant |
| 86 |
|
REAL de_u(klon, klev) ! flux detraine dans le panache montant |
| 87 |
|
REAL en_d(klon, klev) ! flux entraine dans le panache descendant |
| 88 |
|
REAL de_d(klon, klev) ! flux detraine dans le panache descendant |
| 89 |
|
REAL coefh(klon, klev) ! flux detraine dans le panache descendant |
| 90 |
|
|
| 91 |
|
REAL pyu1(klon), pyv1(klon) |
| 92 |
|
REAL pftsol(klon, nbsrf), ppsrf(klon, nbsrf) |
| 93 |
|
REAL pftsol1(klon), pftsol2(klon), pftsol3(klon), pftsol4(klon) |
| 94 |
|
REAL ppsrf1(klon), ppsrf2(klon), ppsrf3(klon), ppsrf4(klon) |
| 95 |
|
|
| 96 |
|
REAL dtcum |
| 97 |
|
|
| 98 |
|
INTEGER:: iadvtr = 0, irec = 1 |
| 99 |
|
REAL zmin, zmax |
| 100 |
|
LOGICAL ok_sync |
| 101 |
|
|
| 102 |
|
SAVE t, mfd, en_u, de_u, en_d, de_d, coefh, dtcum |
| 103 |
|
SAVE fm_therm, entr_therm |
| 104 |
|
SAVE pyu1, pyv1, pftsol, ppsrf |
| 105 |
|
|
| 106 |
|
!------------------------------------------------------ |
| 107 |
|
|
| 108 |
|
! Couche limite: |
| 109 |
|
|
| 110 |
|
ok_sync = .TRUE. |
| 111 |
|
|
| 112 |
|
IF (iadvtr==0) THEN |
| 113 |
|
CALL initphysto('phystoke', rlon, rlat, dtime, dtime*istphy, & |
| 114 |
|
dtime*istphy, physid) |
| 115 |
|
END IF |
| 116 |
|
|
| 117 |
|
i = itap |
| 118 |
|
zx_tmp_2d = gr_phy_write(pphis) |
| 119 |
|
CALL histwrite(physid, 'phis', i, zx_tmp_2d) |
| 120 |
|
|
| 121 |
|
i = itap |
| 122 |
|
zx_tmp_2d = gr_phy_write(paire) |
| 123 |
|
CALL histwrite(physid, 'aire', i, zx_tmp_2d) |
| 124 |
|
|
| 125 |
|
iadvtr = iadvtr + 1 |
| 126 |
|
|
| 127 |
|
IF (mod(iadvtr, istphy) == 1 .OR. istphy == 1) THEN |
| 128 |
|
PRINT *, 'reinitialisation des champs cumules a iadvtr =', iadvtr |
| 129 |
|
DO k = 1, klev |
| 130 |
|
DO i = 1, klon |
| 131 |
|
mfu(i, k) = 0. |
| 132 |
|
mfd(i, k) = 0. |
| 133 |
|
en_u(i, k) = 0. |
| 134 |
|
de_u(i, k) = 0. |
| 135 |
|
en_d(i, k) = 0. |
| 136 |
|
de_d(i, k) = 0. |
| 137 |
|
coefh(i, k) = 0. |
| 138 |
|
t(i, k) = 0. |
| 139 |
|
fm_therm(i, k) = 0. |
| 140 |
|
entr_therm(i, k) = 0. |
| 141 |
|
END DO |
| 142 |
|
END DO |
| 143 |
|
DO i = 1, klon |
| 144 |
|
pyv1(i) = 0. |
| 145 |
|
pyu1(i) = 0. |
| 146 |
|
END DO |
| 147 |
|
DO k = 1, nbsrf |
| 148 |
|
DO i = 1, klon |
| 149 |
|
pftsol(i, k) = 0. |
| 150 |
|
ppsrf(i, k) = 0. |
| 151 |
|
END DO |
| 152 |
|
END DO |
| 153 |
|
|
| 154 |
|
dtcum = 0. |
| 155 |
|
END IF |
| 156 |
|
|
| 157 |
|
DO k = 1, klev |
| 158 |
|
DO i = 1, klon |
| 159 |
|
mfu(i, k) = mfu(i, k) + pmfu(i, k)*pdtphys |
| 160 |
|
mfd(i, k) = mfd(i, k) + pmfd(i, k)*pdtphys |
| 161 |
|
en_u(i, k) = en_u(i, k) + pen_u(i, k)*pdtphys |
| 162 |
|
de_u(i, k) = de_u(i, k) + pde_u(i, k)*pdtphys |
| 163 |
|
en_d(i, k) = en_d(i, k) + pen_d(i, k)*pdtphys |
| 164 |
|
de_d(i, k) = de_d(i, k) + pde_d(i, k)*pdtphys |
| 165 |
|
coefh(i, k) = coefh(i, k) + pcoefh(i, k)*pdtphys |
| 166 |
|
t(i, k) = t(i, k) + pt(i, k)*pdtphys |
| 167 |
|
fm_therm(i, k) = fm_therm(i, k) + pfm_therm(i, k)*pdtphys |
| 168 |
|
entr_therm(i, k) = entr_therm(i, k) + pentr_therm(i, k)*pdtphys |
| 169 |
|
END DO |
| 170 |
|
END DO |
| 171 |
|
DO i = 1, klon |
| 172 |
|
pyv1(i) = pyv1(i) + yv1(i)*pdtphys |
| 173 |
|
pyu1(i) = pyu1(i) + yu1(i)*pdtphys |
| 174 |
|
END DO |
| 175 |
|
DO k = 1, nbsrf |
| 176 |
|
DO i = 1, klon |
| 177 |
|
pftsol(i, k) = pftsol(i, k) + ftsol(i, k)*pdtphys |
| 178 |
|
ppsrf(i, k) = ppsrf(i, k) + pctsrf(i, k)*pdtphys |
| 179 |
|
END DO |
| 180 |
|
END DO |
| 181 |
|
|
| 182 |
|
dtcum = dtcum + pdtphys |
| 183 |
|
|
| 184 |
|
IF (mod(iadvtr, istphy) == 0) THEN |
| 185 |
|
! normalisation par le temps cumule |
| 186 |
|
DO k = 1, klev |
| 187 |
|
DO i = 1, klon |
| 188 |
|
mfu(i, k) = mfu(i, k)/dtcum |
| 189 |
|
mfd(i, k) = mfd(i, k)/dtcum |
| 190 |
|
en_u(i, k) = en_u(i, k)/dtcum |
| 191 |
|
de_u(i, k) = de_u(i, k)/dtcum |
| 192 |
|
en_d(i, k) = en_d(i, k)/dtcum |
| 193 |
|
de_d(i, k) = de_d(i, k)/dtcum |
| 194 |
|
coefh(i, k) = coefh(i, k)/dtcum |
| 195 |
|
! Unitel a enlever |
| 196 |
|
t(i, k) = t(i, k)/dtcum |
| 197 |
|
fm_therm(i, k) = fm_therm(i, k)/dtcum |
| 198 |
|
entr_therm(i, k) = entr_therm(i, k)/dtcum |
| 199 |
|
END DO |
| 200 |
|
END DO |
| 201 |
|
DO i = 1, klon |
| 202 |
|
pyv1(i) = pyv1(i)/dtcum |
| 203 |
|
pyu1(i) = pyu1(i)/dtcum |
| 204 |
|
END DO |
| 205 |
|
DO k = 1, nbsrf |
| 206 |
|
DO i = 1, klon |
| 207 |
|
pftsol(i, k) = pftsol(i, k)/dtcum |
| 208 |
|
pftsol1(i) = pftsol(i, 1) |
| 209 |
|
pftsol2(i) = pftsol(i, 2) |
| 210 |
|
pftsol3(i) = pftsol(i, 3) |
| 211 |
|
pftsol4(i) = pftsol(i, 4) |
| 212 |
|
|
| 213 |
|
ppsrf(i, k) = ppsrf(i, k)/dtcum |
| 214 |
|
ppsrf1(i) = ppsrf(i, 1) |
| 215 |
|
ppsrf2(i) = ppsrf(i, 2) |
| 216 |
|
ppsrf3(i) = ppsrf(i, 3) |
| 217 |
|
ppsrf4(i) = ppsrf(i, 4) |
| 218 |
|
END DO |
| 219 |
|
END DO |
| 220 |
|
|
| 221 |
|
! ecriture des champs |
| 222 |
|
|
| 223 |
|
irec = irec + 1 |
| 224 |
|
|
| 225 |
|
zx_tmp_3d = gr_phy_write(t) |
| 226 |
|
CALL histwrite(physid, 't', itap, zx_tmp_3d) |
| 227 |
|
|
| 228 |
|
zx_tmp_3d = gr_phy_write(mfu) |
| 229 |
|
CALL histwrite(physid, 'mfu', itap, zx_tmp_3d) |
| 230 |
|
zx_tmp_3d = gr_phy_write(mfd) |
| 231 |
|
CALL histwrite(physid, 'mfd', itap, zx_tmp_3d) |
| 232 |
|
zx_tmp_3d = gr_phy_write(en_u) |
| 233 |
|
CALL histwrite(physid, 'en_u', itap, zx_tmp_3d) |
| 234 |
|
zx_tmp_3d = gr_phy_write(de_u) |
| 235 |
|
CALL histwrite(physid, 'de_u', itap, zx_tmp_3d) |
| 236 |
|
zx_tmp_3d = gr_phy_write(en_d) |
| 237 |
|
CALL histwrite(physid, 'en_d', itap, zx_tmp_3d) |
| 238 |
|
zx_tmp_3d = gr_phy_write(de_d) |
| 239 |
|
CALL histwrite(physid, 'de_d', itap, zx_tmp_3d) |
| 240 |
|
zx_tmp_3d = gr_phy_write(coefh) |
| 241 |
|
CALL histwrite(physid, 'coefh', itap, zx_tmp_3d) |
| 242 |
|
|
| 243 |
|
DO k = 1, klev |
| 244 |
|
DO i = 1, klon |
| 245 |
|
fm_therm1(i, k) = fm_therm(i, k) |
| 246 |
|
END DO |
| 247 |
|
END DO |
| 248 |
|
|
| 249 |
|
zx_tmp_3d = gr_phy_write(fm_therm1) |
| 250 |
|
CALL histwrite(physid, 'fm_th', itap, zx_tmp_3d) |
| 251 |
|
|
| 252 |
|
zx_tmp_3d = gr_phy_write(entr_therm) |
| 253 |
|
CALL histwrite(physid, 'en_th', itap, zx_tmp_3d) |
| 254 |
|
!ccc |
| 255 |
|
zx_tmp_3d = gr_phy_write(frac_impa) |
| 256 |
|
CALL histwrite(physid, 'frac_impa', itap, zx_tmp_3d) |
| 257 |
|
|
| 258 |
|
zx_tmp_3d = gr_phy_write(frac_nucl) |
| 259 |
|
CALL histwrite(physid, 'frac_nucl', itap, zx_tmp_3d) |
| 260 |
|
|
| 261 |
|
zx_tmp_2d = gr_phy_write(pyu1) |
| 262 |
|
CALL histwrite(physid, 'pyu1', itap, zx_tmp_2d) |
| 263 |
|
|
| 264 |
|
zx_tmp_2d = gr_phy_write(pyv1) |
| 265 |
|
CALL histwrite(physid, 'pyv1', itap, zx_tmp_2d) |
| 266 |
|
|
| 267 |
|
zx_tmp_2d = gr_phy_write(pftsol1) |
| 268 |
|
CALL histwrite(physid, 'ftsol1', itap, zx_tmp_2d) |
| 269 |
|
zx_tmp_2d = gr_phy_write(pftsol2) |
| 270 |
|
CALL histwrite(physid, 'ftsol2', itap, zx_tmp_2d) |
| 271 |
|
zx_tmp_2d = gr_phy_write(pftsol3) |
| 272 |
|
CALL histwrite(physid, 'ftsol3', itap, zx_tmp_2d) |
| 273 |
|
zx_tmp_2d = gr_phy_write(pftsol4) |
| 274 |
|
CALL histwrite(physid, 'ftsol4', itap, zx_tmp_2d) |
| 275 |
|
|
| 276 |
|
zx_tmp_2d = gr_phy_write(ppsrf1) |
| 277 |
|
CALL histwrite(physid, 'psrf1', itap, zx_tmp_2d) |
| 278 |
|
zx_tmp_2d = gr_phy_write(ppsrf2) |
| 279 |
|
CALL histwrite(physid, 'psrf2', itap, zx_tmp_2d) |
| 280 |
|
zx_tmp_2d = gr_phy_write(ppsrf3) |
| 281 |
|
CALL histwrite(physid, 'psrf3', itap, zx_tmp_2d) |
| 282 |
|
zx_tmp_2d = gr_phy_write(ppsrf4) |
| 283 |
|
CALL histwrite(physid, 'psrf4', itap, zx_tmp_2d) |
| 284 |
|
|
| 285 |
|
IF (ok_sync) CALL histsync(physid) |
| 286 |
|
|
| 287 |
|
! Test sur la valeur des coefficients de lessivage |
| 288 |
|
|
| 289 |
|
zmin = 1E33 |
| 290 |
|
zmax = -1E33 |
| 291 |
|
DO k = 1, klev |
| 292 |
|
DO i = 1, klon |
| 293 |
|
zmax = max(zmax, frac_nucl(i, k)) |
| 294 |
|
zmin = min(zmin, frac_nucl(i, k)) |
| 295 |
|
END DO |
| 296 |
|
END DO |
| 297 |
|
PRINT *, 'coefs de lessivage (min et max)' |
| 298 |
|
PRINT *, 'facteur de nucleation ', zmin, zmax |
| 299 |
|
zmin = 1E33 |
| 300 |
|
zmax = -1E33 |
| 301 |
|
DO k = 1, klev |
| 302 |
|
DO i = 1, klon |
| 303 |
|
zmax = max(zmax, frac_impa(i, k)) |
| 304 |
|
zmin = min(zmin, frac_impa(i, k)) |
| 305 |
|
END DO |
| 306 |
|
END DO |
| 307 |
|
PRINT *, 'facteur d impaction ', zmin, zmax |
| 308 |
|
END IF |
| 309 |
|
|
| 310 |
|
END SUBROUTINE phystokenc |
| 311 |
|
|
| 312 |
|
end module phystokenc_m |
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