| 1 | !> @file diffusion_v.f90 |
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| 2 | !--------------------------------------------------------------------------------! |
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| 3 | ! This file is part of PALM. |
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| 4 | ! |
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| 5 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
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| 6 | ! of the GNU General Public License as published by the Free Software Foundation, |
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| 7 | ! either version 3 of the License, or (at your option) any later version. |
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| 8 | ! |
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| 9 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
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| 10 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
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| 11 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
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| 12 | ! |
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| 13 | ! You should have received a copy of the GNU General Public License along with |
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| 14 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
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| 15 | ! |
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| 16 | ! Copyright 1997-2014 Leibniz Universitaet Hannover |
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| 17 | !--------------------------------------------------------------------------------! |
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| 18 | ! |
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| 19 | ! Current revisions: |
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| 20 | ! ----------------- |
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| 21 | ! unnecessary calculations of kmzm and kmzp in wall bounded parts removed |
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| 22 | ! |
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| 23 | ! Former revisions: |
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| 24 | ! ----------------- |
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| 25 | ! $Id: diffusion_v.f90 1740 2016-01-13 08:19:40Z raasch $ |
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| 26 | ! |
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| 27 | ! 1682 2015-10-07 23:56:08Z knoop |
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| 28 | ! Code annotations made doxygen readable |
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| 29 | ! |
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| 30 | ! 1340 2014-03-25 19:45:13Z kanani |
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| 31 | ! REAL constants defined as wp-kind |
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| 32 | ! |
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| 33 | ! 1320 2014-03-20 08:40:49Z raasch |
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| 34 | ! ONLY-attribute added to USE-statements, |
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| 35 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 36 | ! kinds are defined in new module kinds, |
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| 37 | ! revision history before 2012 removed, |
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| 38 | ! comment fields (!:) to be used for variable explanations added to |
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| 39 | ! all variable declaration statements |
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| 40 | ! |
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| 41 | ! 1257 2013-11-08 15:18:40Z raasch |
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| 42 | ! openacc loop and loop vector clauses removed, declare create moved after |
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| 43 | ! the FORTRAN declaration statement |
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| 44 | ! |
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| 45 | ! 1128 2013-04-12 06:19:32Z raasch |
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| 46 | ! loop index bounds in accelerator version replaced by i_left, i_right, j_south, |
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| 47 | ! j_north |
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| 48 | ! |
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| 49 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 50 | ! code put under GPL (PALM 3.9) |
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| 51 | ! |
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| 52 | ! 1015 2012-09-27 09:23:24Z raasch |
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| 53 | ! accelerator version (*_acc) added |
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| 54 | ! |
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| 55 | ! 1001 2012-09-13 14:08:46Z raasch |
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| 56 | ! arrays comunicated by module instead of parameter list |
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| 57 | ! |
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| 58 | ! 978 2012-08-09 08:28:32Z fricke |
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| 59 | ! outflow damping layer removed |
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| 60 | ! kmxm_x/_y and kmxp_x/_y change to kmxm and kmxp |
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| 61 | ! |
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| 62 | ! Revision 1.1 1997/09/12 06:24:01 raasch |
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| 63 | ! Initial revision |
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| 64 | ! |
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| 65 | ! |
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| 66 | ! Description: |
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| 67 | ! ------------ |
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| 68 | !> Diffusion term of the v-component |
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| 69 | !------------------------------------------------------------------------------! |
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| 70 | MODULE diffusion_v_mod |
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| 71 | |
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| 72 | |
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| 73 | USE wall_fluxes_mod |
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| 74 | |
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| 75 | PRIVATE |
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| 76 | PUBLIC diffusion_v, diffusion_v_acc |
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| 77 | |
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| 78 | INTERFACE diffusion_v |
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| 79 | MODULE PROCEDURE diffusion_v |
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| 80 | MODULE PROCEDURE diffusion_v_ij |
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| 81 | END INTERFACE diffusion_v |
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| 82 | |
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| 83 | INTERFACE diffusion_v_acc |
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| 84 | MODULE PROCEDURE diffusion_v_acc |
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| 85 | END INTERFACE diffusion_v_acc |
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| 86 | |
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| 87 | CONTAINS |
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| 88 | |
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| 89 | |
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| 90 | !------------------------------------------------------------------------------! |
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| 91 | ! Description: |
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| 92 | ! ------------ |
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| 93 | !> Call for all grid points |
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| 94 | !------------------------------------------------------------------------------! |
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| 95 | SUBROUTINE diffusion_v |
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| 96 | |
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| 97 | USE arrays_3d, & |
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| 98 | ONLY: ddzu, ddzw, km, tend, u, v, vsws, vswst, w |
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| 99 | |
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| 100 | USE control_parameters, & |
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| 101 | ONLY: constant_top_momentumflux, topography, use_surface_fluxes, & |
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| 102 | use_top_fluxes |
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| 103 | |
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| 104 | USE grid_variables, & |
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| 105 | ONLY: ddx, ddy, ddy2, fxm, fxp, wall_v |
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| 106 | |
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| 107 | USE indices, & |
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| 108 | ONLY: nxl, nxr, nyn, nys, nysv, nzb, nzb_diff_v, nzb_v_inner, & |
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| 109 | nzb_v_outer, nzt, nzt_diff |
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| 110 | |
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| 111 | USE kinds |
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| 112 | |
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| 113 | IMPLICIT NONE |
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| 114 | |
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| 115 | INTEGER(iwp) :: i !< |
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| 116 | INTEGER(iwp) :: j !< |
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| 117 | INTEGER(iwp) :: k !< |
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| 118 | REAL(wp) :: kmxm !< |
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| 119 | REAL(wp) :: kmxp !< |
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| 120 | REAL(wp) :: kmzm !< |
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| 121 | REAL(wp) :: kmzp !< |
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| 122 | |
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| 123 | REAL(wp), DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: vsus !< |
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| 124 | |
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| 125 | ! |
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| 126 | !-- First calculate horizontal momentum flux v'u' at vertical walls, |
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| 127 | !-- if neccessary |
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| 128 | IF ( topography /= 'flat' ) THEN |
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| 129 | CALL wall_fluxes( vsus, 0.0_wp, 1.0_wp, 0.0_wp, 0.0_wp, nzb_v_inner, & |
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| 130 | nzb_v_outer, wall_v ) |
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| 131 | ENDIF |
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| 132 | |
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| 133 | DO i = nxl, nxr |
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| 134 | DO j = nysv, nyn |
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| 135 | ! |
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| 136 | !-- Compute horizontal diffusion |
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| 137 | DO k = nzb_v_outer(j,i)+1, nzt |
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| 138 | ! |
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| 139 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 140 | kmxp = 0.25_wp * & |
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| 141 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 142 | kmxm = 0.25_wp * & |
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| 143 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 144 | |
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| 145 | tend(k,j,i) = tend(k,j,i) & |
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| 146 | & + ( kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 147 | & + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 148 | & - kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 149 | & - kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 150 | & ) * ddx & |
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| 151 | & + 2.0_wp * ( & |
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| 152 | & km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 153 | & - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 154 | & ) * ddy2 |
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| 155 | ENDDO |
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| 156 | |
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| 157 | ! |
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| 158 | !-- Wall functions at the left and right walls, respectively |
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| 159 | IF ( wall_v(j,i) /= 0.0_wp ) THEN |
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| 160 | |
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| 161 | DO k = nzb_v_inner(j,i)+1, nzb_v_outer(j,i) |
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| 162 | kmxp = 0.25_wp * & |
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| 163 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 164 | kmxm = 0.25_wp * & |
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| 165 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 166 | |
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| 167 | tend(k,j,i) = tend(k,j,i) & |
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| 168 | + 2.0_wp * ( & |
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| 169 | km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 170 | - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 171 | ) * ddy2 & |
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| 172 | + ( fxp(j,i) * ( & |
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| 173 | kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 174 | + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 175 | ) & |
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| 176 | - fxm(j,i) * ( & |
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| 177 | kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 178 | + kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 179 | ) & |
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| 180 | + wall_v(j,i) * vsus(k,j,i) & |
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| 181 | ) * ddx |
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| 182 | ENDDO |
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| 183 | ENDIF |
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| 184 | |
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| 185 | ! |
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| 186 | !-- Compute vertical diffusion. In case of simulating a Prandtl |
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| 187 | !-- layer, index k starts at nzb_v_inner+2. |
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| 188 | DO k = nzb_diff_v(j,i), nzt_diff |
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| 189 | ! |
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| 190 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 191 | kmzp = 0.25_wp * & |
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| 192 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 193 | kmzm = 0.25_wp * & |
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| 194 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 195 | |
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| 196 | tend(k,j,i) = tend(k,j,i) & |
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| 197 | & + ( kmzp * ( ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| 198 | & + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 199 | & ) & |
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| 200 | & - kmzm * ( ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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| 201 | & + ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 202 | & ) & |
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| 203 | & ) * ddzw(k) |
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| 204 | ENDDO |
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| 205 | |
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| 206 | ! |
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| 207 | !-- Vertical diffusion at the first grid point above the surface, |
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| 208 | !-- if the momentum flux at the bottom is given by the Prandtl law |
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| 209 | !-- or if it is prescribed by the user. |
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| 210 | !-- Difference quotient of the momentum flux is not formed over |
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| 211 | !-- half of the grid spacing (2.0*ddzw(k)) any more, since the |
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| 212 | !-- comparison with other (LES) models showed that the values of |
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| 213 | !-- the momentum flux becomes too large in this case. |
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| 214 | !-- The term containing w(k-1,..) (see above equation) is removed here |
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| 215 | !-- because the vertical velocity is assumed to be zero at the surface. |
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| 216 | IF ( use_surface_fluxes ) THEN |
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| 217 | k = nzb_v_inner(j,i)+1 |
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| 218 | ! |
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| 219 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 220 | kmzp = 0.25_wp * & |
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| 221 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 222 | |
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| 223 | tend(k,j,i) = tend(k,j,i) & |
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| 224 | & + ( kmzp * ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 225 | & ) * ddzw(k) & |
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| 226 | & + ( kmzp * ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| 227 | & + vsws(j,i) & |
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| 228 | & ) * ddzw(k) |
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| 229 | ENDIF |
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| 230 | |
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| 231 | ! |
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| 232 | !-- Vertical diffusion at the first gridpoint below the top boundary, |
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| 233 | !-- if the momentum flux at the top is prescribed by the user |
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| 234 | IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN |
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| 235 | k = nzt |
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| 236 | ! |
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| 237 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 238 | kmzm = 0.25_wp * & |
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| 239 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 240 | |
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| 241 | tend(k,j,i) = tend(k,j,i) & |
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| 242 | & - ( kmzm * ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 243 | & ) * ddzw(k) & |
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| 244 | & + ( -vswst(j,i) & |
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| 245 | & - kmzm * ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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| 246 | & ) * ddzw(k) |
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| 247 | ENDIF |
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| 248 | |
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| 249 | ENDDO |
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| 250 | ENDDO |
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| 251 | |
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| 252 | END SUBROUTINE diffusion_v |
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| 253 | |
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| 254 | |
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| 255 | !------------------------------------------------------------------------------! |
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| 256 | ! Description: |
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| 257 | ! ------------ |
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| 258 | !> Call for all grid points - accelerator version |
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| 259 | !------------------------------------------------------------------------------! |
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| 260 | SUBROUTINE diffusion_v_acc |
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| 261 | |
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| 262 | USE arrays_3d, & |
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| 263 | ONLY: ddzu, ddzw, km, tend, u, v, vsws, vswst, w |
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| 264 | |
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| 265 | USE control_parameters, & |
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| 266 | ONLY: constant_top_momentumflux, topography, use_surface_fluxes, & |
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| 267 | use_top_fluxes |
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| 268 | |
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| 269 | USE grid_variables, & |
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| 270 | ONLY: ddx, ddy, ddy2, fxm, fxp, wall_v |
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| 271 | |
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| 272 | USE indices, & |
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| 273 | ONLY: i_left, i_right, j_north, j_south, nxl, nxr, nyn, nys, nzb, & |
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| 274 | nzb_diff_v, nzb_v_inner, nzb_v_outer, nzt, nzt_diff |
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| 275 | |
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| 276 | USE kinds |
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| 277 | |
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| 278 | IMPLICIT NONE |
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| 279 | |
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| 280 | INTEGER(iwp) :: i !< |
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| 281 | INTEGER(iwp) :: j !< |
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| 282 | INTEGER(iwp) :: k !< |
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| 283 | REAL(wp) :: kmxm !< |
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| 284 | REAL(wp) :: kmxp !< |
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| 285 | REAL(wp) :: kmzm !< |
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| 286 | REAL(wp) :: kmzp !< |
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| 287 | |
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| 288 | REAL(wp), DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: vsus !< |
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| 289 | !$acc declare create ( vsus ) |
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| 290 | |
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| 291 | ! |
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| 292 | !-- First calculate horizontal momentum flux v'u' at vertical walls, |
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| 293 | !-- if neccessary |
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| 294 | IF ( topography /= 'flat' ) THEN |
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| 295 | CALL wall_fluxes_acc( vsus, 0.0_wp, 1.0_wp, 0.0_wp, 0.0_wp, & |
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| 296 | nzb_v_inner, nzb_v_outer, wall_v ) |
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| 297 | ENDIF |
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| 298 | |
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| 299 | !$acc kernels present ( u, v, w, km, tend, vsws, vswst ) & |
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| 300 | !$acc present ( ddzu, ddzw, fxm, fxp, wall_v ) & |
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| 301 | !$acc present ( nzb_v_inner, nzb_v_outer, nzb_diff_v ) |
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| 302 | DO i = i_left, i_right |
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| 303 | DO j = j_south, j_north |
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| 304 | ! |
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| 305 | !-- Compute horizontal diffusion |
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| 306 | DO k = 1, nzt |
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| 307 | IF ( k > nzb_v_outer(j,i) ) THEN |
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| 308 | ! |
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| 309 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 310 | kmxp = 0.25_wp * & |
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| 311 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 312 | kmxm = 0.25_wp * & |
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| 313 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 314 | |
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| 315 | tend(k,j,i) = tend(k,j,i) & |
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| 316 | & + ( kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 317 | & + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 318 | & - kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 319 | & - kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 320 | & ) * ddx & |
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| 321 | & + 2.0_wp * ( & |
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| 322 | & km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 323 | & - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 324 | & ) * ddy2 |
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| 325 | ENDIF |
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| 326 | ENDDO |
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| 327 | |
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| 328 | ! |
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| 329 | !-- Wall functions at the left and right walls, respectively |
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| 330 | DO k = 1, nzt |
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| 331 | IF( k > nzb_v_inner(j,i) .AND. k <= nzb_v_outer(j,i) .AND. & |
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| 332 | wall_v(j,i) /= 0.0_wp ) THEN |
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| 333 | |
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| 334 | kmxp = 0.25_wp * & |
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| 335 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 336 | kmxm = 0.25_wp * & |
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| 337 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 338 | |
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| 339 | tend(k,j,i) = tend(k,j,i) & |
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| 340 | + 2.0_wp * ( & |
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| 341 | km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 342 | - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 343 | ) * ddy2 & |
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| 344 | + ( fxp(j,i) * ( & |
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| 345 | kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 346 | + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 347 | ) & |
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| 348 | - fxm(j,i) * ( & |
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| 349 | kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 350 | + kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 351 | ) & |
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| 352 | + wall_v(j,i) * vsus(k,j,i) & |
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| 353 | ) * ddx |
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| 354 | ENDIF |
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| 355 | ENDDO |
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| 356 | |
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| 357 | ! |
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| 358 | !-- Compute vertical diffusion. In case of simulating a Prandtl |
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| 359 | !-- layer, index k starts at nzb_v_inner+2. |
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| 360 | DO k = 1, nzt_diff |
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| 361 | IF ( k >= nzb_diff_v(j,i) ) THEN |
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| 362 | ! |
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| 363 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 364 | kmzp = 0.25_wp * & |
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| 365 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 366 | kmzm = 0.25_wp * & |
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| 367 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 368 | |
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| 369 | tend(k,j,i) = tend(k,j,i) & |
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| 370 | & + ( kmzp * ( ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1)& |
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| 371 | & + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 372 | & ) & |
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| 373 | & - kmzm * ( ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k)& |
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| 374 | & + ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 375 | & ) & |
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| 376 | & ) * ddzw(k) |
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| 377 | ENDIF |
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| 378 | ENDDO |
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| 379 | |
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| 380 | ENDDO |
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| 381 | ENDDO |
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| 382 | |
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| 383 | ! |
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| 384 | !-- Vertical diffusion at the first grid point above the surface, |
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| 385 | !-- if the momentum flux at the bottom is given by the Prandtl law |
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| 386 | !-- or if it is prescribed by the user. |
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| 387 | !-- Difference quotient of the momentum flux is not formed over |
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| 388 | !-- half of the grid spacing (2.0*ddzw(k)) any more, since the |
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| 389 | !-- comparison with other (LES) models showed that the values of |
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| 390 | !-- the momentum flux becomes too large in this case. |
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| 391 | !-- The term containing w(k-1,..) (see above equation) is removed here |
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| 392 | !-- because the vertical velocity is assumed to be zero at the surface. |
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| 393 | IF ( use_surface_fluxes ) THEN |
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| 394 | |
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| 395 | DO i = i_left, i_right |
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| 396 | DO j = j_south, j_north |
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| 397 | |
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| 398 | k = nzb_v_inner(j,i)+1 |
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| 399 | ! |
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| 400 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 401 | kmzp = 0.25_wp * & |
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| 402 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 403 | |
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| 404 | tend(k,j,i) = tend(k,j,i) & |
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| 405 | & + ( kmzp * ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 406 | & ) * ddzw(k) & |
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| 407 | & + ( kmzp * ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| 408 | & + vsws(j,i) & |
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| 409 | & ) * ddzw(k) |
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| 410 | ENDDO |
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| 411 | ENDDO |
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| 412 | |
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| 413 | ENDIF |
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| 414 | |
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| 415 | ! |
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| 416 | !-- Vertical diffusion at the first gridpoint below the top boundary, |
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| 417 | !-- if the momentum flux at the top is prescribed by the user |
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| 418 | IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN |
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| 419 | |
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| 420 | k = nzt |
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| 421 | |
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| 422 | DO i = i_left, i_right |
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| 423 | DO j = j_south, j_north |
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| 424 | |
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| 425 | ! |
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| 426 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 427 | kmzm = 0.25_wp * & |
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| 428 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 429 | |
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| 430 | tend(k,j,i) = tend(k,j,i) & |
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| 431 | & - ( kmzm * ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 432 | & ) * ddzw(k) & |
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| 433 | & + ( -vswst(j,i) & |
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| 434 | & - kmzm * ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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| 435 | & ) * ddzw(k) |
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| 436 | ENDDO |
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| 437 | ENDDO |
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| 438 | |
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| 439 | ENDIF |
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| 440 | !$acc end kernels |
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| 441 | |
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| 442 | END SUBROUTINE diffusion_v_acc |
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| 443 | |
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| 444 | |
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| 445 | !------------------------------------------------------------------------------! |
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| 446 | ! Description: |
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| 447 | ! ------------ |
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| 448 | !> Call for grid point i,j |
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| 449 | !------------------------------------------------------------------------------! |
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| 450 | SUBROUTINE diffusion_v_ij( i, j ) |
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| 451 | |
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| 452 | USE arrays_3d, & |
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| 453 | ONLY: ddzu, ddzw, km, tend, u, v, vsws, vswst, w |
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| 454 | |
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| 455 | USE control_parameters, & |
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| 456 | ONLY: constant_top_momentumflux, use_surface_fluxes, use_top_fluxes |
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| 457 | |
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| 458 | USE grid_variables, & |
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| 459 | ONLY: ddx, ddy, ddy2, fxm, fxp, wall_v |
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| 460 | |
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| 461 | USE indices, & |
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| 462 | ONLY: nzb, nzb_diff_v, nzb_v_inner, nzb_v_outer, nzt, nzt_diff |
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| 463 | |
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| 464 | USE kinds |
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| 465 | |
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| 466 | IMPLICIT NONE |
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| 467 | |
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| 468 | INTEGER(iwp) :: i !< |
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| 469 | INTEGER(iwp) :: j !< |
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| 470 | INTEGER(iwp) :: k !< |
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| 471 | REAL(wp) :: kmxm !< |
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| 472 | REAL(wp) :: kmxp !< |
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| 473 | REAL(wp) :: kmzm !< |
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| 474 | REAL(wp) :: kmzp !< |
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| 475 | |
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| 476 | REAL(wp), DIMENSION(nzb:nzt+1) :: vsus !< |
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| 477 | |
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| 478 | ! |
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| 479 | !-- Compute horizontal diffusion |
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| 480 | DO k = nzb_v_outer(j,i)+1, nzt |
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| 481 | ! |
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| 482 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 483 | kmxp = 0.25_wp * ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 484 | kmxm = 0.25_wp * ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 485 | |
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| 486 | tend(k,j,i) = tend(k,j,i) & |
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| 487 | & + ( kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 488 | & + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 489 | & - kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 490 | & - kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 491 | & ) * ddx & |
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| 492 | & + 2.0_wp * ( & |
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| 493 | & km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 494 | & - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 495 | & ) * ddy2 |
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| 496 | ENDDO |
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| 497 | |
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| 498 | ! |
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| 499 | !-- Wall functions at the left and right walls, respectively |
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| 500 | IF ( wall_v(j,i) /= 0.0_wp ) THEN |
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| 501 | |
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| 502 | ! |
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| 503 | !-- Calculate the horizontal momentum flux v'u' |
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| 504 | CALL wall_fluxes( i, j, nzb_v_inner(j,i)+1, nzb_v_outer(j,i), & |
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| 505 | vsus, 0.0_wp, 1.0_wp, 0.0_wp, 0.0_wp ) |
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| 506 | |
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| 507 | DO k = nzb_v_inner(j,i)+1, nzb_v_outer(j,i) |
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| 508 | kmxp = 0.25_wp * & |
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| 509 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 510 | kmxm = 0.25_wp * & |
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| 511 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 512 | |
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| 513 | tend(k,j,i) = tend(k,j,i) & |
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| 514 | + 2.0_wp * ( & |
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| 515 | km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 516 | - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 517 | ) * ddy2 & |
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| 518 | + ( fxp(j,i) * ( & |
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| 519 | kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 520 | + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 521 | ) & |
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| 522 | - fxm(j,i) * ( & |
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| 523 | kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 524 | + kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 525 | ) & |
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| 526 | + wall_v(j,i) * vsus(k) & |
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| 527 | ) * ddx |
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| 528 | ENDDO |
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| 529 | ENDIF |
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| 530 | |
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| 531 | ! |
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| 532 | !-- Compute vertical diffusion. In case of simulating a Prandtl layer, |
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| 533 | !-- index k starts at nzb_v_inner+2. |
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| 534 | DO k = nzb_diff_v(j,i), nzt_diff |
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| 535 | ! |
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| 536 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 537 | kmzp = 0.25_wp * ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 538 | kmzm = 0.25_wp * ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 539 | |
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| 540 | tend(k,j,i) = tend(k,j,i) & |
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| 541 | & + ( kmzp * ( ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| 542 | & + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 543 | & ) & |
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| 544 | & - kmzm * ( ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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| 545 | & + ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 546 | & ) & |
|---|
| 547 | & ) * ddzw(k) |
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| 548 | ENDDO |
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| 549 | |
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| 550 | ! |
|---|
| 551 | !-- Vertical diffusion at the first grid point above the surface, if the |
|---|
| 552 | !-- momentum flux at the bottom is given by the Prandtl law or if it is |
|---|
| 553 | !-- prescribed by the user. |
|---|
| 554 | !-- Difference quotient of the momentum flux is not formed over half of |
|---|
| 555 | !-- the grid spacing (2.0*ddzw(k)) any more, since the comparison with |
|---|
| 556 | !-- other (LES) models showed that the values of the momentum flux becomes |
|---|
| 557 | !-- too large in this case. |
|---|
| 558 | !-- The term containing w(k-1,..) (see above equation) is removed here |
|---|
| 559 | !-- because the vertical velocity is assumed to be zero at the surface. |
|---|
| 560 | IF ( use_surface_fluxes ) THEN |
|---|
| 561 | k = nzb_v_inner(j,i)+1 |
|---|
| 562 | ! |
|---|
| 563 | !-- Interpolate eddy diffusivities on staggered gridpoints |
|---|
| 564 | kmzp = 0.25_wp * ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 565 | |
|---|
| 566 | tend(k,j,i) = tend(k,j,i) & |
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| 567 | & + ( kmzp * ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 568 | & ) * ddzw(k) & |
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| 569 | & + ( kmzp * ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| 570 | & + vsws(j,i) & |
|---|
| 571 | & ) * ddzw(k) |
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| 572 | ENDIF |
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| 573 | |
|---|
| 574 | ! |
|---|
| 575 | !-- Vertical diffusion at the first gridpoint below the top boundary, |
|---|
| 576 | !-- if the momentum flux at the top is prescribed by the user |
|---|
| 577 | IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN |
|---|
| 578 | k = nzt |
|---|
| 579 | ! |
|---|
| 580 | !-- Interpolate eddy diffusivities on staggered gridpoints |
|---|
| 581 | kmzm = 0.25_wp * & |
|---|
| 582 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
|---|
| 583 | |
|---|
| 584 | tend(k,j,i) = tend(k,j,i) & |
|---|
| 585 | & - ( kmzm * ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
|---|
| 586 | & ) * ddzw(k) & |
|---|
| 587 | & + ( -vswst(j,i) & |
|---|
| 588 | & - kmzm * ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
|---|
| 589 | & ) * ddzw(k) |
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| 590 | ENDIF |
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| 591 | |
|---|
| 592 | END SUBROUTINE diffusion_v_ij |
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| 593 | |
|---|
| 594 | END MODULE diffusion_v_mod |
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