source: LMDZ6/trunk/libf/dyn3d/friction.f90 @ 5300

!
! $Id: friction.f90 5292 2024-10-28 15:58:32Z abarral $
!
!=======================================================================
SUBROUTINE friction(ucov,vcov,pdt)
  USE iniprint_mod_h
  USE comgeom2_mod_h
  USE control_mod
  USE IOIPSL
  USE comconst_mod, ONLY: pi
  USE dimensions_mod, ONLY: iim, jjm, llm, ndm
  USE paramet_mod_h
  USE academic_mod_h, ONLY: kfrict
IMPLICIT NONE

  !=======================================================================
  !
  !   Friction for the Newtonian case:
  !   --------------------------------
  !    2 possibilities (depending on flag 'friction_type'
  ! friction_type=0 : A friction that is only applied to the lowermost
  !                   atmospheric layer
  ! friction_type=1 : Friction applied on all atmospheric layer (but
  !   (default)       with stronger magnitude near the surface; see
  !                   iniacademic.F)
  !=======================================================================

  ! arguments:
  REAL,INTENT(out) :: ucov( iip1,jjp1,llm )
  REAL,INTENT(out) :: vcov( iip1,jjm,llm )
  REAL,INTENT(in) :: pdt ! time step

  ! local variables:

  REAL :: modv(iip1,jjp1),zco,zsi
  REAL :: vpn,vps,upoln,upols,vpols,vpoln
  REAL :: u2(iip1,jjp1),v2(iip1,jjm)
  INTEGER :: i,j,l
  REAL,PARAMETER :: cfric=1.e-5
  LOGICAL,SAVE :: firstcall=.true.
  INTEGER,SAVE :: friction_type=1
  CHARACTER(len=20) :: modname="friction"
  CHARACTER(len=80) :: abort_message

  IF (firstcall) THEN
    ! ! set friction type
    call getin("friction_type",friction_type)
    if ((friction_type.lt.0).or.(friction_type.gt.1)) then
      abort_message="wrong friction type"
      write(lunout,*)'Friction: wrong friction type',friction_type
      call abort_gcm(modname,abort_message,42)
    endif
    firstcall=.false.
  ENDIF

  if (friction_type.eq.0) then
  !   calcul des composantes au carre du vent naturel
  do j=1,jjp1
     do i=1,iip1
        u2(i,j)=ucov(i,j,1)*ucov(i,j,1)*unscu2(i,j)
     enddo
  enddo
  do j=1,jjm
     do i=1,iip1
        v2(i,j)=vcov(i,j,1)*vcov(i,j,1)*unscv2(i,j)
     enddo
  enddo

  !   calcul du module de V en dehors des poles
  do j=2,jjm
     do i=2,iip1
        modv(i,j)=sqrt(0.5*(u2(i-1,j)+u2(i,j)+v2(i,j-1)+v2(i,j)))
     enddo
     modv(1,j)=modv(iip1,j)
  enddo

  !   les deux composantes du vent au pole sont obtenues comme
  !   premiers modes de fourier de v pres du pole
  upoln=0.
  vpoln=0.
  upols=0.
  vpols=0.
  do i=2,iip1
     zco=cos(rlonv(i))*(rlonu(i)-rlonu(i-1))
     zsi=sin(rlonv(i))*(rlonu(i)-rlonu(i-1))
     vpn=vcov(i,1,1)/cv(i,1)
     vps=vcov(i,jjm,1)/cv(i,jjm)
     upoln=upoln+zco*vpn
     vpoln=vpoln+zsi*vpn
     upols=upols+zco*vps
     vpols=vpols+zsi*vps
  enddo
  vpn=sqrt(upoln*upoln+vpoln*vpoln)/pi
  vps=sqrt(upols*upols+vpols*vpols)/pi
  do i=1,iip1
     ! modv(i,1)=vpn
     ! modv(i,jjp1)=vps
     modv(i,1)=modv(i,2)
     modv(i,jjp1)=modv(i,jjm)
  enddo

  !   calcul du frottement au sol.
  do j=2,jjm
     do i=1,iim
        ucov(i,j,1)=ucov(i,j,1) &
              -cfric*pdt*0.5*(modv(i+1,j)+modv(i,j))*ucov(i,j,1)
     enddo
     ucov(iip1,j,1)=ucov(1,j,1)
  enddo
  do j=1,jjm
     do i=1,iip1
        vcov(i,j,1)=vcov(i,j,1) &
              -cfric*pdt*0.5*(modv(i,j+1)+modv(i,j))*vcov(i,j,1)
     enddo
     vcov(iip1,j,1)=vcov(1,j,1)
  enddo
  endif ! of if (friction_type.eq.0)

  if (friction_type.eq.1) then
    do l=1,llm
      ucov(:,:,l)=ucov(:,:,l)*(1.-pdt*kfrict(l))
      vcov(:,:,l)=vcov(:,:,l)*(1.-pdt*kfrict(l))
    enddo
  endif

  RETURN
END SUBROUTINE friction