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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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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) |
| 314 |
|
|
CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol4, zx_tmp_2d) |
| 315 |
|
|
CALL histwrite(physid,"ftsol4",itap,zx_tmp_2d, |
| 316 |
|
|
. iim*(jjm+1),ndex2d) |
| 317 |
|
|
|
| 318 |
|
|
CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf1, zx_tmp_2d) |
| 319 |
|
|
CALL histwrite(physid,"psrf1",itap,zx_tmp_2d, |
| 320 |
|
|
. iim*(jjm+1),ndex2d) |
| 321 |
|
|
CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf2, zx_tmp_2d) |
| 322 |
|
|
CALL histwrite(physid,"psrf2",itap,zx_tmp_2d, |
| 323 |
|
|
. iim*(jjm+1),ndex2d) |
| 324 |
|
|
CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf3, zx_tmp_2d) |
| 325 |
|
|
CALL histwrite(physid,"psrf3",itap,zx_tmp_2d, |
| 326 |
|
|
. iim*(jjm+1),ndex2d) |
| 327 |
|
|
CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf4, zx_tmp_2d) |
| 328 |
|
|
CALL histwrite(physid,"psrf4",itap,zx_tmp_2d, |
| 329 |
|
|
. iim*(jjm+1),ndex2d) |
| 330 |
|
|
|
| 331 |
|
|
if (ok_sync) call histsync(physid) |
| 332 |
|
|
c if (ok_sync) call histsync |
| 333 |
|
|
|
| 334 |
|
|
c |
| 335 |
|
|
cAA Test sur la valeur des coefficients de lessivage |
| 336 |
|
|
c |
| 337 |
|
|
zmin=1e33 |
| 338 |
|
|
zmax=-1e33 |
| 339 |
|
|
do k=1,klev |
| 340 |
|
|
do i=1,klon |
| 341 |
|
|
zmax=max(zmax,frac_nucl(i,k)) |
| 342 |
|
|
zmin=min(zmin,frac_nucl(i,k)) |
| 343 |
|
|
enddo |
| 344 |
|
|
enddo |
| 345 |
|
|
Print*,'------ coefs de lessivage (min et max) --------' |
| 346 |
|
|
Print*,'facteur de nucleation ',zmin,zmax |
| 347 |
|
|
zmin=1e33 |
| 348 |
|
|
zmax=-1e33 |
| 349 |
|
|
do k=1,klev |
| 350 |
|
|
do i=1,klon |
| 351 |
|
|
zmax=max(zmax,frac_impa(i,k)) |
| 352 |
|
|
zmin=min(zmin,frac_impa(i,k)) |
| 353 |
|
|
enddo |
| 354 |
|
|
enddo |
| 355 |
|
|
Print*,'facteur d impaction ',zmin,zmax |
| 356 |
|
|
|
| 357 |
|
|
ENDIF |
| 358 |
|
|
|
| 359 |
|
|
c reinitialisation des champs cumules |
| 360 |
|
|
go to 768 |
| 361 |
|
|
if (mod(iadvtr,istphy).eq.1) then |
| 362 |
|
|
do k=1,klev |
| 363 |
|
|
do i=1,klon |
| 364 |
|
|
mfu(i,k)=0. |
| 365 |
|
|
mfd(i,k)=0. |
| 366 |
|
|
en_u(i,k)=0. |
| 367 |
|
|
de_u(i,k)=0. |
| 368 |
|
|
en_d(i,k)=0. |
| 369 |
|
|
de_d(i,k)=0. |
| 370 |
|
|
coefh(i,k)=0. |
| 371 |
|
|
t(i,k)=0. |
| 372 |
|
|
fm_therm(i,k)=0. |
| 373 |
|
|
entr_therm(i,k)=0. |
| 374 |
|
|
enddo |
| 375 |
|
|
enddo |
| 376 |
|
|
do i=1,klon |
| 377 |
|
|
pyv1(i)=0. |
| 378 |
|
|
pyu1(i)=0. |
| 379 |
|
|
end do |
| 380 |
|
|
do k=1,nbsrf |
| 381 |
|
|
do i=1,klon |
| 382 |
|
|
pftsol(i,k)=0. |
| 383 |
|
|
ppsrf(i,k)=0. |
| 384 |
|
|
enddo |
| 385 |
|
|
enddo |
| 386 |
|
|
|
| 387 |
|
|
dtcum=0. |
| 388 |
|
|
endif |
| 389 |
|
|
|
| 390 |
|
|
do k=1,klev |
| 391 |
|
|
do i=1,klon |
| 392 |
|
|
mfu(i,k)=mfu(i,k)+pmfu(i,k)*pdtphys |
| 393 |
|
|
mfd(i,k)=mfd(i,k)+pmfd(i,k)*pdtphys |
| 394 |
|
|
en_u(i,k)=en_u(i,k)+pen_u(i,k)*pdtphys |
| 395 |
|
|
de_u(i,k)=de_u(i,k)+pde_u(i,k)*pdtphys |
| 396 |
|
|
en_d(i,k)=en_d(i,k)+pen_d(i,k)*pdtphys |
| 397 |
|
|
de_d(i,k)=de_d(i,k)+pde_d(i,k)*pdtphys |
| 398 |
|
|
coefh(i,k)=coefh(i,k)+pcoefh(i,k)*pdtphys |
| 399 |
|
|
t(i,k)=t(i,k)+pt(i,k)*pdtphys |
| 400 |
|
|
fm_therm(i,k)=fm_therm(i,k)+pfm_therm(i,k)*pdtphys |
| 401 |
|
|
entr_therm(i,k)=entr_therm(i,k)+pentr_therm(i,k)*pdtphys |
| 402 |
|
|
enddo |
| 403 |
|
|
enddo |
| 404 |
|
|
do i=1,klon |
| 405 |
|
|
pyv1(i)=pyv1(i)+yv1(i)*pdtphys |
| 406 |
|
|
pyu1(i)=pyu1(i)+yu1(i)*pdtphys |
| 407 |
|
|
end do |
| 408 |
|
|
do k=1,nbsrf |
| 409 |
|
|
do i=1,klon |
| 410 |
|
|
pftsol(i,k)=pftsol(i,k)+ftsol(i,k)*pdtphys |
| 411 |
|
|
ppsrf(i,k)=ppsrf(i,k)+pctsrf(i,k)*pdtphys |
| 412 |
|
|
enddo |
| 413 |
|
|
enddo |
| 414 |
|
|
|
| 415 |
|
|
dtcum=dtcum+pdtphys |
| 416 |
|
|
768 continue |
| 417 |
|
|
|
| 418 |
|
|
RETURN |
| 419 |
|
|
END |
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