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! $Id: friction.F 2597 2016-07-22 06:44:47Z emillour $ |
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c======================================================================= |
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SUBROUTINE friction(ucov,vcov,pdt) |
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USE control_mod |
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#ifdef CPP_IOIPSL |
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USE IOIPSL |
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#else |
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! if not using IOIPSL, we still need to use (a local version of) getin |
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USE ioipsl_getincom |
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#endif |
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USE comconst_mod, ONLY: pi |
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IMPLICIT NONE |
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!======================================================================= |
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! |
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! Friction for the Newtonian case: |
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! -------------------------------- |
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! 2 possibilities (depending on flag 'friction_type' |
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! friction_type=0 : A friction that is only applied to the lowermost |
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! atmospheric layer |
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! friction_type=1 : Friction applied on all atmospheric layer (but |
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! (default) with stronger magnitude near the surface; see |
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! iniacademic.F) |
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!======================================================================= |
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include "dimensions.h" |
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include "paramet.h" |
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include "comgeom2.h" |
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include "iniprint.h" |
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include "academic.h" |
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! arguments: |
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REAL,INTENT(out) :: ucov( iip1,jjp1,llm ) |
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REAL,INTENT(out) :: vcov( iip1,jjm,llm ) |
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REAL,INTENT(in) :: pdt ! time step |
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! local variables: |
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REAL modv(iip1,jjp1),zco,zsi |
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REAL vpn,vps,upoln,upols,vpols,vpoln |
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REAL u2(iip1,jjp1),v2(iip1,jjm) |
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INTEGER i,j,l |
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REAL,PARAMETER :: cfric=1.e-5 |
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LOGICAL,SAVE :: firstcall=.true. |
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INTEGER,SAVE :: friction_type=1 |
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CHARACTER(len=20) :: modname="friction" |
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CHARACTER(len=80) :: abort_message |
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IF (firstcall) THEN |
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! set friction type |
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call getin("friction_type",friction_type) |
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if ((friction_type.lt.0).or.(friction_type.gt.1)) then |
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abort_message="wrong friction type" |
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write(lunout,*)'Friction: wrong friction type',friction_type |
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call abort_gcm(modname,abort_message,42) |
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endif |
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firstcall=.false. |
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ENDIF |
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if (friction_type.eq.0) then |
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c calcul des composantes au carre du vent naturel |
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do j=1,jjp1 |
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do i=1,iip1 |
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u2(i,j)=ucov(i,j,1)*ucov(i,j,1)*unscu2(i,j) |
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enddo |
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enddo |
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do j=1,jjm |
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do i=1,iip1 |
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v2(i,j)=vcov(i,j,1)*vcov(i,j,1)*unscv2(i,j) |
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enddo |
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enddo |
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c calcul du module de V en dehors des poles |
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do j=2,jjm |
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do i=2,iip1 |
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modv(i,j)=sqrt(0.5*(u2(i-1,j)+u2(i,j)+v2(i,j-1)+v2(i,j))) |
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enddo |
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modv(1,j)=modv(iip1,j) |
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enddo |
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c les deux composantes du vent au pole sont obtenues comme |
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c premiers modes de fourier de v pres du pole |
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upoln=0. |
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vpoln=0. |
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upols=0. |
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vpols=0. |
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do i=2,iip1 |
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zco=cos(rlonv(i))*(rlonu(i)-rlonu(i-1)) |
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zsi=sin(rlonv(i))*(rlonu(i)-rlonu(i-1)) |
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vpn=vcov(i,1,1)/cv(i,1) |
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vps=vcov(i,jjm,1)/cv(i,jjm) |
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upoln=upoln+zco*vpn |
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vpoln=vpoln+zsi*vpn |
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upols=upols+zco*vps |
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vpols=vpols+zsi*vps |
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enddo |
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vpn=sqrt(upoln*upoln+vpoln*vpoln)/pi |
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vps=sqrt(upols*upols+vpols*vpols)/pi |
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do i=1,iip1 |
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c modv(i,1)=vpn |
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c modv(i,jjp1)=vps |
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modv(i,1)=modv(i,2) |
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modv(i,jjp1)=modv(i,jjm) |
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enddo |
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c calcul du frottement au sol. |
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do j=2,jjm |
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do i=1,iim |
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ucov(i,j,1)=ucov(i,j,1) |
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s -cfric*pdt*0.5*(modv(i+1,j)+modv(i,j))*ucov(i,j,1) |
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enddo |
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ucov(iip1,j,1)=ucov(1,j,1) |
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enddo |
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do j=1,jjm |
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do i=1,iip1 |
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vcov(i,j,1)=vcov(i,j,1) |
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s -cfric*pdt*0.5*(modv(i,j+1)+modv(i,j))*vcov(i,j,1) |
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enddo |
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vcov(iip1,j,1)=vcov(1,j,1) |
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enddo |
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endif ! of if (friction_type.eq.0) |
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if (friction_type.eq.1) then |
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do l=1,llm |
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ucov(:,:,l)=ucov(:,:,l)*(1.-pdt*kfrict(l)) |
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vcov(:,:,l)=vcov(:,:,l)*(1.-pdt*kfrict(l)) |
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enddo |
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endif |
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RETURN |
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END |
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