lmdz_spla_neutral.f90 Source File


Files dependent on this one

sourcefile~~lmdz_spla_neutral.f90~~AfferentGraph sourcefile~lmdz_spla_neutral.f90 lmdz_spla_neutral.f90 sourcefile~lmdz_spla_nightingale.f90 lmdz_spla_nightingale.f90 sourcefile~lmdz_spla_nightingale.f90->sourcefile~lmdz_spla_neutral.f90 sourcefile~lmdz_spla_nightingale.f90~2 lmdz_spla_nightingale.f90 sourcefile~lmdz_spla_nightingale.f90~2->sourcefile~lmdz_spla_neutral.f90 sourcefile~precuremission.f90 precuremission.f90 sourcefile~precuremission.f90->sourcefile~lmdz_spla_nightingale.f90 sourcefile~precuremission.f90~2 precuremission.f90 sourcefile~precuremission.f90~2->sourcefile~lmdz_spla_nightingale.f90

Contents

Source Code


Source Code

MODULE lmdz_spla_neutral
  CONTAINS
!***********************************************************************
  subroutine spla_neutral(klon,u10_mps,ustar_mps,obklen_m, &
          u10n_mps )
  !-----------------------------------------------------------------------	
  ! subroutine to compute u10 neutral wind speed
  ! inputs
  ! u10_mps - wind speed at 10 m (m/s)
  ! ustar_mps - friction velocity (m/s)
  ! obklen_m - monin-obukhov length scale (m)
  ! outputs
  ! u10n_mps - wind speed at 10 m under neutral conditions (m/s)
  ! following code assumes reference height Z is 10m, consistent with use
  ! of u10 and u10_neutral.  If not, code
  ! should be changed so that constants of 50. and 160. in equations
  ! below are changed to -5 * Z and -16 * Z respectively.
  ! Reference:  G. L. Geernaert.  'Bulk parameterizations for the
  ! wind stress and heat fluxes,' in Surface Waves and Fluxes, Vol. I,
  ! Current Theory, Geernaert and W.J. Plant, editors, Kluwer Academic
  ! Publishers, Boston, MA, 1990.
  ! subroutine written Feb 2001 by eg chapman
  ! adapted to LMD-ZT by E. Cosme 310801
  ! Following Will Shaw (PNL, Seattle) the theory applied for flux
  ! calculation with the scheme of Nightingale et al. (2000) does not
  ! hold anymore when -1<obklen<20. In this case, u10n is set to 0,
  ! so that the transfer velocity  computed in nightingale.F will also
  ! be 0. The flux is then set to 0.
  !----------------------------------------------------------------------		
  !
  !
  IMPLICIT NONE
  !
  INTEGER, intent(in) :: klon  

    
    real, dimension(klon), intent(in) :: u10_mps, ustar_mps, obklen_m
    real, dimension(klon), intent(out) :: u10n_mps
    real :: pi,von_karman
    ! parameter (pi = 3.141592653589793, von_karman = 0.4)	
  ! pour etre coherent avec vk de bl_for_dms.F
    parameter (pi = 3.141592653589793, von_karman = 0.35)
  !
    real :: phi, phi_inv, phi_inv_sq, f1, f2, f3, dum1, psi
    integer :: i


    psi = 0.
    do i=1,klon
    ! Original : needs u10_mps defined as "inout" to be able to modify it here, but in reality it is only "in"
    !if (u10_mps(i) .lt. 0.) u10_mps(i) = 0.0
    ! Instead, STOP to check why the module is negative
    if (u10_mps(i) .lt. 0.) STOP 'negative wind module u10 in input of spla_neutral' 

    if  (obklen_m(i) .lt. 0.) then
            phi = (1. - 160./obklen_m(i))**(-0.25)
            phi_inv = 1./phi
            phi_inv_sq = 1./phi * 1./phi
            f1 = (1. + phi_inv) / 2.
            f2 = (1. + phi_inv_sq)/2.
  ! following to avoid numerical overruns. recall tan(90deg)=infinity
            dum1 = min (1.e24, phi_inv)
            f3 = atan(dum1)
            psi = 2.*log(f1) + log(f2) - 2.*f3 + pi/2.
    else if (obklen_m(i) .gt. 0.) then
            psi = -50. / obklen_m(i)
    end if

    u10n_mps(i) = u10_mps(i) + (ustar_mps(i) * psi /von_karman )
  ! u10n set to 0. if -1 < obklen < 20
    if ((obklen_m(i).gt.-1.).and.(obklen_m(i).lt.20.)) then
        u10n_mps(i) = 0.
    endif
    if (u10n_mps(i) .lt. 0.) u10n_mps(i) = 0.0

    enddo
    return
end subroutine spla_neutral
!***********************************************************************
END MODULE lmdz_spla_neutral