!> @file diffusion_u.f90 !--------------------------------------------------------------------------------! ! This file is part of PALM. ! ! PALM is free software: you can redistribute it and/or modify it under the terms ! of the GNU General Public License as published by the Free Software Foundation, ! either version 3 of the License, or (at your option) any later version. ! ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. ! ! You should have received a copy of the GNU General Public License along with ! PALM. If not, see . ! ! Copyright 1997-2015 Leibniz Universitaet Hannover !--------------------------------------------------------------------------------! ! ! Current revisions: ! ----------------- ! ! ! Former revisions: ! ----------------- ! $Id: diffusion_u.f90 1692 2015-10-26 16:29:17Z boeske $ ! ! 1691 2015-10-26 16:17:44Z maronga ! Formatting corrections. ! ! 1682 2015-10-07 23:56:08Z knoop ! Code annotations made doxygen readable ! ! 1340 2014-03-25 19:45:13Z kanani ! REAL constants defined as wp-kind ! ! 1320 2014-03-20 08:40:49Z raasch ! ONLY-attribute added to USE-statements, ! kind-parameters added to all INTEGER and REAL declaration statements, ! kinds are defined in new module kinds, ! revision history before 2012 removed, ! comment fields (!:) to be used for variable explanations added to ! all variable declaration statements ! ! 1257 2013-11-08 15:18:40Z raasch ! openacc loop and loop vector clauses removed, declare create moved after ! the FORTRAN declaration statement ! ! 1128 2013-04-12 06:19:32Z raasch ! loop index bounds in accelerator version replaced by i_left, i_right, j_south, ! j_north ! ! 1036 2012-10-22 13:43:42Z raasch ! code put under GPL (PALM 3.9) ! ! 1015 2012-09-27 09:23:24Z raasch ! accelerator version (*_acc) added ! ! 1001 2012-09-13 14:08:46Z raasch ! arrays comunicated by module instead of parameter list ! ! 978 2012-08-09 08:28:32Z fricke ! outflow damping layer removed ! kmym_x/_y and kmyp_x/_y change to kmym and kmyp ! ! Revision 1.1 1997/09/12 06:23:51 raasch ! Initial revision ! ! ! Description: ! ------------ !> Diffusion term of the u-component !> @todo additional damping (needed for non-cyclic bc) causes bad vectorization !> and slows down the speed on NEC about 5-10% !------------------------------------------------------------------------------! MODULE diffusion_u_mod USE wall_fluxes_mod PRIVATE PUBLIC diffusion_u, diffusion_u_acc INTERFACE diffusion_u MODULE PROCEDURE diffusion_u MODULE PROCEDURE diffusion_u_ij END INTERFACE diffusion_u INTERFACE diffusion_u_acc MODULE PROCEDURE diffusion_u_acc END INTERFACE diffusion_u_acc CONTAINS !------------------------------------------------------------------------------! ! Description: ! ------------ !> Call for all grid points !------------------------------------------------------------------------------! SUBROUTINE diffusion_u USE arrays_3d, & ONLY: ddzu, ddzw, km, tend, u, usws, uswst, v, w USE control_parameters, & ONLY: constant_top_momentumflux, topography, use_surface_fluxes, & use_top_fluxes USE grid_variables, & ONLY: ddx, ddx2, ddy, fym, fyp, wall_u USE indices, & ONLY: nxl, nxlu, nxr, nyn, nys, nzb, nzb_diff_u, nzb_u_inner, & nzb_u_outer, nzt, nzt_diff USE kinds IMPLICIT NONE INTEGER(iwp) :: i !< INTEGER(iwp) :: j !< INTEGER(iwp) :: k !< REAL(wp) :: kmym !< REAL(wp) :: kmyp !< REAL(wp) :: kmzm !< REAL(wp) :: kmzp !< REAL(wp), DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: usvs !< ! !-- First calculate horizontal momentum flux u'v' at vertical walls, !-- if neccessary IF ( topography /= 'flat' ) THEN CALL wall_fluxes( usvs, 1.0_wp, 0.0_wp, 0.0_wp, 0.0_wp, nzb_u_inner, & nzb_u_outer, wall_u ) ENDIF DO i = nxlu, nxr DO j = nys, nyn ! !-- Compute horizontal diffusion DO k = nzb_u_outer(j,i)+1, nzt ! !-- Interpolate eddy diffusivities on staggered gridpoints kmyp = 0.25_wp * & ( km(k,j,i)+km(k,j+1,i)+km(k,j,i-1)+km(k,j+1,i-1) ) kmym = 0.25_wp * & ( km(k,j,i)+km(k,j-1,i)+km(k,j,i-1)+km(k,j-1,i-1) ) tend(k,j,i) = tend(k,j,i) & & + 2.0_wp * ( & & km(k,j,i) * ( u(k,j,i+1) - u(k,j,i) ) & & - km(k,j,i-1) * ( u(k,j,i) - u(k,j,i-1) ) & & ) * ddx2 & & + ( kmyp * ( u(k,j+1,i) - u(k,j,i) ) * ddy & & + kmyp * ( v(k,j+1,i) - v(k,j+1,i-1) ) * ddx & & - kmym * ( u(k,j,i) - u(k,j-1,i) ) * ddy & & - kmym * ( v(k,j,i) - v(k,j,i-1) ) * ddx & & ) * ddy ENDDO ! !-- Wall functions at the north and south walls, respectively IF ( wall_u(j,i) /= 0.0_wp ) THEN DO k = nzb_u_inner(j,i)+1, nzb_u_outer(j,i) kmyp = 0.25_wp * & ( km(k,j,i)+km(k,j+1,i)+km(k,j,i-1)+km(k,j+1,i-1) ) kmym = 0.25_wp * & ( km(k,j,i)+km(k,j-1,i)+km(k,j,i-1)+km(k,j-1,i-1) ) tend(k,j,i) = tend(k,j,i) & + 2.0_wp * ( & km(k,j,i) * ( u(k,j,i+1) - u(k,j,i) ) & - km(k,j,i-1) * ( u(k,j,i) - u(k,j,i-1) ) & ) * ddx2 & + ( fyp(j,i) * ( & kmyp * ( u(k,j+1,i) - u(k,j,i) ) * ddy & + kmyp * ( v(k,j+1,i) - v(k,j+1,i-1) ) * ddx & ) & - fym(j,i) * ( & kmym * ( u(k,j,i) - u(k,j-1,i) ) * ddy & + kmym * ( v(k,j,i) - v(k,j,i-1) ) * ddx & ) & + wall_u(j,i) * usvs(k,j,i) & ) * ddy ENDDO ENDIF ! !-- Compute vertical diffusion. In case of simulating a Prandtl layer, !-- index k starts at nzb_u_inner+2. DO k = nzb_diff_u(j,i), nzt_diff ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * & ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * & ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & + ( kmzp * ( ( u(k+1,j,i) - u(k,j,i) ) * ddzu(k+1) & & + ( w(k,j,i) - w(k,j,i-1) ) * ddx & & ) & & - kmzm * ( ( u(k,j,i) - u(k-1,j,i) ) * ddzu(k) & & + ( w(k-1,j,i) - w(k-1,j,i-1) ) * ddx & & ) & & ) * ddzw(k) ENDDO ! !-- Vertical diffusion at the first grid point above the surface, !-- if the momentum flux at the bottom is given by the Prandtl law or !-- if it is prescribed by the user. !-- Difference quotient of the momentum flux is not formed over half !-- of the grid spacing (2.0*ddzw(k)) any more, since the comparison !-- with other (LES) models showed that the values of the momentum !-- flux becomes too large in this case. !-- The term containing w(k-1,..) (see above equation) is removed here !-- because the vertical velocity is assumed to be zero at the surface. IF ( use_surface_fluxes ) THEN k = nzb_u_inner(j,i)+1 ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * & ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * & ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & + ( kmzp * ( w(k,j,i) - w(k,j,i-1) ) * ddx & & ) * ddzw(k) & & + ( kmzp * ( u(k+1,j,i) - u(k,j,i) ) * ddzu(k+1) & & + usws(j,i) & & ) * ddzw(k) ENDIF ! !-- Vertical diffusion at the first gridpoint below the top boundary, !-- if the momentum flux at the top is prescribed by the user IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN k = nzt ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * & ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * & ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & - ( kmzm * ( w(k-1,j,i) - w(k-1,j,i-1) ) * ddx & & ) * ddzw(k) & & + ( -uswst(j,i) & & - kmzm * ( u(k,j,i) - u(k-1,j,i) ) * ddzu(k) & & ) * ddzw(k) ENDIF ENDDO ENDDO END SUBROUTINE diffusion_u !------------------------------------------------------------------------------! ! Description: ! ------------ !> Call for all grid points - accelerator version !------------------------------------------------------------------------------! SUBROUTINE diffusion_u_acc USE arrays_3d, & ONLY: ddzu, ddzw, km, tend, u, usws, uswst, v, w USE control_parameters, & ONLY: constant_top_momentumflux, topography, use_surface_fluxes, & use_top_fluxes USE grid_variables, & ONLY: ddx, ddx2, ddy, fym, fyp, wall_u USE indices, & ONLY: i_left, i_right, j_north, j_south, nxl, nxr, nyn, nys, nzb, & nzb_diff_u, nzb_u_inner, nzb_u_outer, nzt, nzt_diff USE kinds IMPLICIT NONE INTEGER(iwp) :: i !< INTEGER(iwp) :: j !< INTEGER(iwp) :: k !< REAL(wp) :: kmym !< REAL(wp) :: kmyp !< REAL(wp) :: kmzm !< REAL(wp) :: kmzp !< REAL(wp), DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: usvs !< !$acc declare create ( usvs ) ! !-- First calculate horizontal momentum flux u'v' at vertical walls, !-- if neccessary IF ( topography /= 'flat' ) THEN CALL wall_fluxes_acc( usvs, 1.0_wp, 0.0_wp, 0.0_wp, 0.0_wp, & nzb_u_inner, nzb_u_outer, wall_u ) ENDIF !$acc kernels present ( u, v, w, km, tend, usws, uswst ) & !$acc present ( ddzu, ddzw, fym, fyp, wall_u ) & !$acc present ( nzb_u_inner, nzb_u_outer, nzb_diff_u ) DO i = i_left, i_right DO j = j_south, j_north ! !-- Compute horizontal diffusion DO k = 1, nzt IF ( k > nzb_u_outer(j,i) ) THEN ! !-- Interpolate eddy diffusivities on staggered gridpoints kmyp = 0.25_wp * & ( km(k,j,i)+km(k,j+1,i)+km(k,j,i-1)+km(k,j+1,i-1) ) kmym = 0.25_wp * & ( km(k,j,i)+km(k,j-1,i)+km(k,j,i-1)+km(k,j-1,i-1) ) tend(k,j,i) = tend(k,j,i) & & + 2.0_wp * ( & & km(k,j,i) * ( u(k,j,i+1) - u(k,j,i) ) & & - km(k,j,i-1) * ( u(k,j,i) - u(k,j,i-1) ) & & ) * ddx2 & & + ( kmyp * ( u(k,j+1,i) - u(k,j,i) ) * ddy & & + kmyp * ( v(k,j+1,i) - v(k,j+1,i-1) ) * ddx & & - kmym * ( u(k,j,i) - u(k,j-1,i) ) * ddy & & - kmym * ( v(k,j,i) - v(k,j,i-1) ) * ddx & & ) * ddy ENDIF ENDDO ! !-- Wall functions at the north and south walls, respectively DO k = 1, nzt IF( k > nzb_u_inner(j,i) .AND. k <= nzb_u_outer(j,i) .AND. & wall_u(j,i) /= 0.0_wp ) THEN kmyp = 0.25_wp * & ( km(k,j,i)+km(k,j+1,i)+km(k,j,i-1)+km(k,j+1,i-1) ) kmym = 0.25_wp * & ( km(k,j,i)+km(k,j-1,i)+km(k,j,i-1)+km(k,j-1,i-1) ) tend(k,j,i) = tend(k,j,i) & + 2.0_wp * ( & km(k,j,i) * ( u(k,j,i+1) - u(k,j,i) ) & - km(k,j,i-1) * ( u(k,j,i) - u(k,j,i-1) ) & ) * ddx2 & + ( fyp(j,i) * ( & kmyp * ( u(k,j+1,i) - u(k,j,i) ) * ddy & + kmyp * ( v(k,j+1,i) - v(k,j+1,i-1) ) * ddx & ) & - fym(j,i) * ( & kmym * ( u(k,j,i) - u(k,j-1,i) ) * ddy & + kmym * ( v(k,j,i) - v(k,j,i-1) ) * ddx & ) & + wall_u(j,i) * usvs(k,j,i) & ) * ddy ENDIF ENDDO ! !-- Compute vertical diffusion. In case of simulating a Prandtl layer, !-- index k starts at nzb_u_inner+2. DO k = 1, nzt_diff IF ( k >= nzb_diff_u(j,i) ) THEN ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * & ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * & ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & + ( kmzp * ( ( u(k+1,j,i) - u(k,j,i) ) * ddzu(k+1)& & + ( w(k,j,i) - w(k,j,i-1) ) * ddx & & ) & & - kmzm * ( ( u(k,j,i) - u(k-1,j,i) ) * ddzu(k)& & + ( w(k-1,j,i) - w(k-1,j,i-1) ) * ddx & & ) & & ) * ddzw(k) ENDIF ENDDO ENDDO ENDDO ! !-- Vertical diffusion at the first grid point above the surface, !-- if the momentum flux at the bottom is given by the Prandtl law or !-- if it is prescribed by the user. !-- Difference quotient of the momentum flux is not formed over half !-- of the grid spacing (2.0*ddzw(k)) any more, since the comparison !-- with other (LES) models showed that the values of the momentum !-- flux becomes too large in this case. !-- The term containing w(k-1,..) (see above equation) is removed here !-- because the vertical velocity is assumed to be zero at the surface. IF ( use_surface_fluxes ) THEN DO i = i_left, i_right DO j = j_south, j_north k = nzb_u_inner(j,i)+1 ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * & ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * & ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & + ( kmzp * ( w(k,j,i) - w(k,j,i-1) ) * ddx & & ) * ddzw(k) & & + ( kmzp * ( u(k+1,j,i) - u(k,j,i) ) * ddzu(k+1) & & + usws(j,i) & & ) * ddzw(k) ENDDO ENDDO ENDIF ! !-- Vertical diffusion at the first gridpoint below the top boundary, !-- if the momentum flux at the top is prescribed by the user IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN k = nzt DO i = i_left, i_right DO j = j_south, j_north ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * & ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * & ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & - ( kmzm * ( w(k-1,j,i) - w(k-1,j,i-1) ) * ddx & & ) * ddzw(k) & & + ( -uswst(j,i) & & - kmzm * ( u(k,j,i) - u(k-1,j,i) ) * ddzu(k) & & ) * ddzw(k) ENDDO ENDDO ENDIF !$acc end kernels END SUBROUTINE diffusion_u_acc !------------------------------------------------------------------------------! ! Description: ! ------------ !> Call for grid point i,j !------------------------------------------------------------------------------! SUBROUTINE diffusion_u_ij( i, j ) USE arrays_3d, & ONLY: ddzu, ddzw, km, tend, u, usws, uswst, v, w USE control_parameters, & ONLY: constant_top_momentumflux, use_surface_fluxes, use_top_fluxes USE grid_variables, & ONLY: ddx, ddx2, ddy, fym, fyp, wall_u USE indices, & ONLY: nzb, nzb_diff_u, nzb_u_inner, nzb_u_outer, nzt, nzt_diff USE kinds IMPLICIT NONE INTEGER(iwp) :: i !< INTEGER(iwp) :: j !< INTEGER(iwp) :: k !< REAL(wp) :: kmym !< REAL(wp) :: kmyp !< REAL(wp) :: kmzm !< REAL(wp) :: kmzp !< REAL(wp), DIMENSION(nzb:nzt+1) :: usvs !< ! !-- Compute horizontal diffusion DO k = nzb_u_outer(j,i)+1, nzt ! !-- Interpolate eddy diffusivities on staggered gridpoints kmyp = 0.25_wp * ( km(k,j,i)+km(k,j+1,i)+km(k,j,i-1)+km(k,j+1,i-1) ) kmym = 0.25_wp * ( km(k,j,i)+km(k,j-1,i)+km(k,j,i-1)+km(k,j-1,i-1) ) tend(k,j,i) = tend(k,j,i) & & + 2.0_wp * ( & & km(k,j,i) * ( u(k,j,i+1) - u(k,j,i) ) & & - km(k,j,i-1) * ( u(k,j,i) - u(k,j,i-1) ) & & ) * ddx2 & & + ( kmyp * ( u(k,j+1,i) - u(k,j,i) ) * ddy & & + kmyp * ( v(k,j+1,i) - v(k,j+1,i-1) ) * ddx & & - kmym * ( u(k,j,i) - u(k,j-1,i) ) * ddy & & - kmym * ( v(k,j,i) - v(k,j,i-1) ) * ddx & & ) * ddy ENDDO ! !-- Wall functions at the north and south walls, respectively IF ( wall_u(j,i) /= 0.0_wp ) THEN ! !-- Calculate the horizontal momentum flux u'v' CALL wall_fluxes( i, j, nzb_u_inner(j,i)+1, nzb_u_outer(j,i), & usvs, 1.0_wp, 0.0_wp, 0.0_wp, 0.0_wp ) DO k = nzb_u_inner(j,i)+1, nzb_u_outer(j,i) kmyp = 0.25_wp * ( km(k,j,i)+km(k,j+1,i)+km(k,j,i-1)+km(k,j+1,i-1) ) kmym = 0.25_wp * ( km(k,j,i)+km(k,j-1,i)+km(k,j,i-1)+km(k,j-1,i-1) ) tend(k,j,i) = tend(k,j,i) & + 2.0_wp * ( & km(k,j,i) * ( u(k,j,i+1) - u(k,j,i) ) & - km(k,j,i-1) * ( u(k,j,i) - u(k,j,i-1) ) & ) * ddx2 & + ( fyp(j,i) * ( & kmyp * ( u(k,j+1,i) - u(k,j,i) ) * ddy & + kmyp * ( v(k,j+1,i) - v(k,j+1,i-1) ) * ddx & ) & - fym(j,i) * ( & kmym * ( u(k,j,i) - u(k,j-1,i) ) * ddy & + kmym * ( v(k,j,i) - v(k,j,i-1) ) * ddx & ) & + wall_u(j,i) * usvs(k) & ) * ddy ENDDO ENDIF ! !-- Compute vertical diffusion. In case of simulating a Prandtl layer, !-- index k starts at nzb_u_inner+2. DO k = nzb_diff_u(j,i), nzt_diff ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & + ( kmzp * ( ( u(k+1,j,i) - u(k,j,i) ) * ddzu(k+1) & & + ( w(k,j,i) - w(k,j,i-1) ) * ddx & & ) & & - kmzm * ( ( u(k,j,i) - u(k-1,j,i) ) * ddzu(k) & & + ( w(k-1,j,i) - w(k-1,j,i-1) ) * ddx & & ) & & ) * ddzw(k) ENDDO ! !-- Vertical diffusion at the first grid point above the surface, if the !-- momentum flux at the bottom is given by the Prandtl law or if it is !-- prescribed by the user. !-- Difference quotient of the momentum flux is not formed over half of !-- the grid spacing (2.0*ddzw(k)) any more, since the comparison with !-- other (LES) models showed that the values of the momentum flux becomes !-- too large in this case. !-- The term containing w(k-1,..) (see above equation) is removed here !-- because the vertical velocity is assumed to be zero at the surface. IF ( use_surface_fluxes ) THEN k = nzb_u_inner(j,i)+1 ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & + ( kmzp * ( w(k,j,i) - w(k,j,i-1) ) * ddx & & ) * ddzw(k) & & + ( kmzp * ( u(k+1,j,i) - u(k,j,i) ) * ddzu(k+1) & & + usws(j,i) & & ) * ddzw(k) ENDIF ! !-- Vertical diffusion at the first gridpoint below the top boundary, !-- if the momentum flux at the top is prescribed by the user IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN k = nzt ! !-- Interpolate eddy diffusivities on staggered gridpoints kmzp = 0.25_wp * & ( km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) ) kmzm = 0.25_wp * & ( km(k,j,i)+km(k-1,j,i)+km(k,j,i-1)+km(k-1,j,i-1) ) tend(k,j,i) = tend(k,j,i) & & - ( kmzm * ( w(k-1,j,i) - w(k-1,j,i-1) ) * ddx & & ) * ddzw(k) & & + ( -uswst(j,i) & & - kmzm * ( u(k,j,i) - u(k-1,j,i) ) * ddzu(k) & & ) * ddzw(k) ENDIF END SUBROUTINE diffusion_u_ij END MODULE diffusion_u_mod