[56] | 1 | MODULE wall_fluxes_mod |
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[1036] | 2 | |
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| 3 | !--------------------------------------------------------------------------------! |
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| 4 | ! This file is part of PALM. |
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| 5 | ! |
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| 6 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
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| 7 | ! of the GNU General Public License as published by the Free Software Foundation, |
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| 8 | ! either version 3 of the License, or (at your option) any later version. |
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| 9 | ! |
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| 10 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
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| 11 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
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| 12 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
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| 13 | ! |
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| 14 | ! You should have received a copy of the GNU General Public License along with |
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| 15 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
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| 16 | ! |
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[1310] | 17 | ! Copyright 1997-2014 Leibniz Universitaet Hannover |
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[1036] | 18 | !--------------------------------------------------------------------------------! |
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| 19 | ! |
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[484] | 20 | ! Current revisions: |
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[52] | 21 | ! ----------------- |
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[198] | 22 | ! |
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[1258] | 23 | ! |
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[198] | 24 | ! Former revisions: |
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| 25 | ! ----------------- |
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| 26 | ! $Id: wall_fluxes.f90 1310 2014-03-14 08:01:56Z heinze $ |
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| 27 | ! |
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[1258] | 28 | ! 1257 2013-11-08 15:18:40Z raasch |
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| 29 | ! openacc loop and loop vector clauses removed |
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| 30 | ! |
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[1154] | 31 | ! 1153 2013-05-10 14:33:08Z raasch |
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| 32 | ! code adjustments of accelerator version required by PGI 12.3 / CUDA 5.0 |
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| 33 | ! |
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[1132] | 34 | ! 1128 2013-04-12 06:19:32Z raasch |
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| 35 | ! loop index bounds in accelerator version replaced by i_left, i_right, j_south, |
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| 36 | ! j_north |
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| 37 | ! |
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[1037] | 38 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 39 | ! code put under GPL (PALM 3.9) |
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| 40 | ! |
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[1017] | 41 | ! 1015 2012-09-27 09:23:24Z raasch |
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| 42 | ! accelerator version (*_acc) added |
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| 43 | ! |
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[198] | 44 | ! 187 2008-08-06 16:25:09Z letzel |
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| 45 | ! Bugfix: Modification of the evaluation of the vertical turbulent momentum |
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| 46 | ! fluxes u'w' and v'w (see prandtl_fluxes), this requires the calculation of |
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| 47 | ! us_wall (and vel_total, u_i, v_i, ws) also in wall_fluxes_e. |
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| 48 | ! Bugfix: change definition of us_wall from 1D to 2D |
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[187] | 49 | ! Bugfix: storage of rifs to rifs_wall in wall_fluxes_e removed |
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| 50 | ! Change: add 'minus' sign to fluxes produced by subroutine wall_fluxes_e for |
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[198] | 51 | ! consistency with subroutine wall_fluxes |
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[187] | 52 | ! Change: Modification of the integrated version of the profile function for |
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[198] | 53 | ! momentum for unstable stratification |
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[52] | 54 | ! |
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| 55 | ! Initial version (2007/03/07) |
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| 56 | ! |
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| 57 | ! Description: |
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| 58 | ! ------------ |
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| 59 | ! Calculates momentum fluxes at vertical walls assuming Monin-Obukhov |
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| 60 | ! similarity. |
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| 61 | ! Indices: usvs a=1, vsus b=1, wsvs c1=1, wsus c2=1 (other=0). |
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[56] | 62 | ! The all-gridpoint version of wall_fluxes_e is not used so far, because |
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| 63 | ! it gives slightly different results from the ij-version for some unknown |
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| 64 | ! reason. |
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[52] | 65 | !------------------------------------------------------------------------------! |
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[56] | 66 | PRIVATE |
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[1015] | 67 | PUBLIC wall_fluxes, wall_fluxes_acc, wall_fluxes_e, wall_fluxes_e_acc |
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[56] | 68 | |
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| 69 | INTERFACE wall_fluxes |
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| 70 | MODULE PROCEDURE wall_fluxes |
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| 71 | MODULE PROCEDURE wall_fluxes_ij |
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| 72 | END INTERFACE wall_fluxes |
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| 73 | |
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[1015] | 74 | INTERFACE wall_fluxes_acc |
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| 75 | MODULE PROCEDURE wall_fluxes_acc |
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| 76 | END INTERFACE wall_fluxes_acc |
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| 77 | |
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[56] | 78 | INTERFACE wall_fluxes_e |
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| 79 | MODULE PROCEDURE wall_fluxes_e |
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| 80 | MODULE PROCEDURE wall_fluxes_e_ij |
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| 81 | END INTERFACE wall_fluxes_e |
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| 82 | |
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[1015] | 83 | INTERFACE wall_fluxes_e_acc |
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| 84 | MODULE PROCEDURE wall_fluxes_e_acc |
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| 85 | END INTERFACE wall_fluxes_e_acc |
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| 86 | |
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[56] | 87 | CONTAINS |
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[52] | 88 | |
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[56] | 89 | !------------------------------------------------------------------------------! |
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| 90 | ! Call for all grid points |
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| 91 | !------------------------------------------------------------------------------! |
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[75] | 92 | SUBROUTINE wall_fluxes( wall_flux, a, b, c1, c2, nzb_uvw_inner, & |
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[56] | 93 | nzb_uvw_outer, wall ) |
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[52] | 94 | |
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[56] | 95 | USE arrays_3d |
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| 96 | USE control_parameters |
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| 97 | USE grid_variables |
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| 98 | USE indices |
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| 99 | USE statistics |
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[52] | 100 | |
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[56] | 101 | IMPLICIT NONE |
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[52] | 102 | |
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[75] | 103 | INTEGER :: i, j, k, wall_index |
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[52] | 104 | |
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[667] | 105 | INTEGER, DIMENSION(nysg:nyng,nxlg:nxrg) :: nzb_uvw_inner, & |
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[56] | 106 | nzb_uvw_outer |
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| 107 | REAL :: a, b, c1, c2, h1, h2, zp |
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| 108 | REAL :: pts, pt_i, rifs, u_i, v_i, us_wall, vel_total, ws, wspts |
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[52] | 109 | |
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[667] | 110 | REAL, DIMENSION(nysg:nyng,nxlg:nxrg) :: wall |
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[75] | 111 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
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[52] | 112 | |
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| 113 | |
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[56] | 114 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 115 | wall_flux = 0.0 |
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| 116 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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| 117 | |
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[75] | 118 | DO i = nxl, nxr |
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| 119 | DO j = nys, nyn |
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[56] | 120 | |
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| 121 | IF ( wall(j,i) /= 0.0 ) THEN |
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[52] | 122 | ! |
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[56] | 123 | !-- All subsequent variables are computed for the respective |
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[187] | 124 | !-- location where the respective flux is defined. |
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[56] | 125 | DO k = nzb_uvw_inner(j,i)+1, nzb_uvw_outer(j,i) |
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[53] | 126 | |
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[52] | 127 | ! |
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[56] | 128 | !-- (1) Compute rifs, u_i, v_i, ws, pt' and w'pt' |
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| 129 | rifs = rif_wall(k,j,i,wall_index) |
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[53] | 130 | |
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[56] | 131 | u_i = a * u(k,j,i) + c1 * 0.25 * & |
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| 132 | ( u(k+1,j,i+1) + u(k+1,j,i) + u(k,j,i+1) + u(k,j,i) ) |
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[53] | 133 | |
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[56] | 134 | v_i = b * v(k,j,i) + c2 * 0.25 * & |
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| 135 | ( v(k+1,j+1,i) + v(k+1,j,i) + v(k,j+1,i) + v(k,j,i) ) |
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[53] | 136 | |
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[56] | 137 | ws = ( c1 + c2 ) * w(k,j,i) + 0.25 * ( & |
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| 138 | a * ( w(k-1,j,i-1) + w(k-1,j,i) + w(k,j,i-1) + w(k,j,i) ) & |
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| 139 | + b * ( w(k-1,j-1,i) + w(k-1,j,i) + w(k,j-1,i) + w(k,j,i) ) & |
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| 140 | ) |
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| 141 | pt_i = 0.5 * ( pt(k,j,i) + a * pt(k,j,i-1) + & |
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| 142 | b * pt(k,j-1,i) + ( c1 + c2 ) * pt(k+1,j,i) ) |
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[53] | 143 | |
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[56] | 144 | pts = pt_i - hom(k,1,4,0) |
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| 145 | wspts = ws * pts |
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[53] | 146 | |
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[52] | 147 | ! |
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[56] | 148 | !-- (2) Compute wall-parallel absolute velocity vel_total |
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| 149 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
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[53] | 150 | |
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[52] | 151 | ! |
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[56] | 152 | !-- (3) Compute wall friction velocity us_wall |
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| 153 | IF ( rifs >= 0.0 ) THEN |
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[53] | 154 | |
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[52] | 155 | ! |
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[56] | 156 | !-- Stable stratification (and neutral) |
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| 157 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 158 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 159 | ) |
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| 160 | ELSE |
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[53] | 161 | |
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[52] | 162 | ! |
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[56] | 163 | !-- Unstable stratification |
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[187] | 164 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 165 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[53] | 166 | |
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[187] | 167 | us_wall = kappa * vel_total / ( & |
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| 168 | LOG( zp / z0(j,i) ) - & |
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| 169 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 170 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 171 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 172 | ) |
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[56] | 173 | ENDIF |
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[53] | 174 | |
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[52] | 175 | ! |
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[56] | 176 | !-- (4) Compute zp/L (corresponds to neutral Richardson flux |
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| 177 | !-- number rifs) |
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| 178 | rifs = -1.0 * zp * kappa * g * wspts / ( pt_i * & |
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| 179 | ( us_wall**3 + 1E-30 ) ) |
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[53] | 180 | |
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[52] | 181 | ! |
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[56] | 182 | !-- Limit the value range of the Richardson numbers. |
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| 183 | !-- This is necessary for very small velocities (u,w --> 0), |
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| 184 | !-- because the absolute value of rif can then become very |
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| 185 | !-- large, which in consequence would result in very large |
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| 186 | !-- shear stresses and very small momentum fluxes (both are |
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| 187 | !-- generally unrealistic). |
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| 188 | IF ( rifs < rif_min ) rifs = rif_min |
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| 189 | IF ( rifs > rif_max ) rifs = rif_max |
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[53] | 190 | |
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[52] | 191 | ! |
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[56] | 192 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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| 193 | IF ( rifs >= 0.0 ) THEN |
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[53] | 194 | |
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[52] | 195 | ! |
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[56] | 196 | !-- Stable stratification (and neutral) |
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| 197 | wall_flux(k,j,i) = kappa * & |
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| 198 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / & |
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| 199 | ( LOG( zp / z0(j,i) ) + & |
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| 200 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 201 | ) |
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| 202 | ELSE |
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[53] | 203 | |
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[52] | 204 | ! |
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[56] | 205 | !-- Unstable stratification |
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[187] | 206 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 207 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[53] | 208 | |
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[187] | 209 | wall_flux(k,j,i) = kappa * & |
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| 210 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / ( & |
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| 211 | LOG( zp / z0(j,i) ) - & |
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| 212 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 213 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 214 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 215 | ) |
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[56] | 216 | ENDIF |
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[187] | 217 | wall_flux(k,j,i) = -wall_flux(k,j,i) * us_wall |
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[56] | 218 | |
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| 219 | ! |
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| 220 | !-- store rifs for next time step |
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| 221 | rif_wall(k,j,i,wall_index) = rifs |
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| 222 | |
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| 223 | ENDDO |
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| 224 | |
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| 225 | ENDIF |
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| 226 | |
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| 227 | ENDDO |
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| 228 | ENDDO |
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| 229 | |
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| 230 | END SUBROUTINE wall_fluxes |
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| 231 | |
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| 232 | |
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[1015] | 233 | !------------------------------------------------------------------------------! |
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| 234 | ! Call for all grid points - accelerator version |
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| 235 | !------------------------------------------------------------------------------! |
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| 236 | SUBROUTINE wall_fluxes_acc( wall_flux, a, b, c1, c2, nzb_uvw_inner, & |
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| 237 | nzb_uvw_outer, wall ) |
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[56] | 238 | |
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[1015] | 239 | USE arrays_3d |
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| 240 | USE control_parameters |
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| 241 | USE grid_variables |
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| 242 | USE indices |
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| 243 | USE statistics |
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| 244 | |
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| 245 | IMPLICIT NONE |
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| 246 | |
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| 247 | INTEGER :: i, j, k, max_outer, min_inner, wall_index |
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| 248 | |
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| 249 | INTEGER, DIMENSION(nysg:nyng,nxlg:nxrg) :: nzb_uvw_inner, & |
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| 250 | nzb_uvw_outer |
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| 251 | REAL :: a, b, c1, c2, h1, h2, zp |
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| 252 | REAL :: pts, pt_i, rifs, u_i, v_i, us_wall, vel_total, ws, wspts |
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| 253 | |
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| 254 | REAL, DIMENSION(nysg:nyng,nxlg:nxrg) :: wall |
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| 255 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
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| 256 | |
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| 257 | |
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| 258 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 259 | wall_flux = 0.0 |
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| 260 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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| 261 | |
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| 262 | min_inner = MINVAL( nzb_uvw_inner(nys:nyn,nxl:nxr) ) + 1 |
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| 263 | max_outer = MINVAL( nzb_uvw_outer(nys:nyn,nxl:nxr) ) |
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| 264 | |
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| 265 | !$acc kernels present( hom, nzb_uvw_inner, nzb_uvw_outer, pt, rif_wall ) & |
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| 266 | !$acc present( u, v, w, wall, wall_flux, z0 ) |
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[1153] | 267 | !$acc loop independent |
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[1128] | 268 | DO i = i_left, i_right |
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| 269 | DO j = j_south, j_north |
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[1153] | 270 | |
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| 271 | IF ( wall(j,i) /= 0.0 ) THEN |
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[1015] | 272 | ! |
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| 273 | !-- All subsequent variables are computed for the respective |
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| 274 | !-- location where the respective flux is defined. |
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[1257] | 275 | !$acc loop independent |
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[1153] | 276 | DO k = nzb_uvw_inner(j,i)+1, nzb_uvw_outer(j,i) |
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| 277 | |
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[1015] | 278 | ! |
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| 279 | !-- (1) Compute rifs, u_i, v_i, ws, pt' and w'pt' |
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| 280 | rifs = rif_wall(k,j,i,wall_index) |
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| 281 | |
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| 282 | u_i = a * u(k,j,i) + c1 * 0.25 * & |
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| 283 | ( u(k+1,j,i+1) + u(k+1,j,i) + u(k,j,i+1) + u(k,j,i) ) |
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| 284 | |
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| 285 | v_i = b * v(k,j,i) + c2 * 0.25 * & |
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| 286 | ( v(k+1,j+1,i) + v(k+1,j,i) + v(k,j+1,i) + v(k,j,i) ) |
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| 287 | |
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| 288 | ws = ( c1 + c2 ) * w(k,j,i) + 0.25 * ( & |
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| 289 | a * ( w(k-1,j,i-1) + w(k-1,j,i) + w(k,j,i-1) + w(k,j,i) ) & |
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| 290 | + b * ( w(k-1,j-1,i) + w(k-1,j,i) + w(k,j-1,i) + w(k,j,i) ) & |
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| 291 | ) |
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| 292 | pt_i = 0.5 * ( pt(k,j,i) + a * pt(k,j,i-1) + & |
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| 293 | b * pt(k,j-1,i) + ( c1 + c2 ) * pt(k+1,j,i) ) |
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| 294 | |
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| 295 | pts = pt_i - hom(k,1,4,0) |
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| 296 | wspts = ws * pts |
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| 297 | |
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| 298 | ! |
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| 299 | !-- (2) Compute wall-parallel absolute velocity vel_total |
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| 300 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
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| 301 | |
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| 302 | ! |
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| 303 | !-- (3) Compute wall friction velocity us_wall |
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| 304 | IF ( rifs >= 0.0 ) THEN |
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| 305 | |
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| 306 | ! |
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| 307 | !-- Stable stratification (and neutral) |
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| 308 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 309 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 310 | ) |
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| 311 | ELSE |
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| 312 | |
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| 313 | ! |
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| 314 | !-- Unstable stratification |
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| 315 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 316 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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| 317 | |
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| 318 | us_wall = kappa * vel_total / ( & |
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| 319 | LOG( zp / z0(j,i) ) - & |
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| 320 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 321 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 322 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 323 | ) |
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| 324 | ENDIF |
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| 325 | |
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| 326 | ! |
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| 327 | !-- (4) Compute zp/L (corresponds to neutral Richardson flux |
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| 328 | !-- number rifs) |
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| 329 | rifs = -1.0 * zp * kappa * g * wspts / ( pt_i * & |
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| 330 | ( us_wall**3 + 1E-30 ) ) |
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| 331 | |
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| 332 | ! |
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| 333 | !-- Limit the value range of the Richardson numbers. |
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| 334 | !-- This is necessary for very small velocities (u,w --> 0), |
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| 335 | !-- because the absolute value of rif can then become very |
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| 336 | !-- large, which in consequence would result in very large |
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| 337 | !-- shear stresses and very small momentum fluxes (both are |
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| 338 | !-- generally unrealistic). |
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| 339 | IF ( rifs < rif_min ) rifs = rif_min |
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| 340 | IF ( rifs > rif_max ) rifs = rif_max |
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| 341 | |
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| 342 | ! |
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| 343 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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| 344 | IF ( rifs >= 0.0 ) THEN |
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| 345 | |
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| 346 | ! |
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| 347 | !-- Stable stratification (and neutral) |
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| 348 | wall_flux(k,j,i) = kappa * & |
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| 349 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / & |
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| 350 | ( LOG( zp / z0(j,i) ) + & |
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| 351 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 352 | ) |
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| 353 | ELSE |
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| 354 | |
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| 355 | ! |
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| 356 | !-- Unstable stratification |
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| 357 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 358 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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| 359 | |
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| 360 | wall_flux(k,j,i) = kappa * & |
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| 361 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / ( & |
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| 362 | LOG( zp / z0(j,i) ) - & |
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| 363 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 364 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 365 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 366 | ) |
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| 367 | ENDIF |
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| 368 | wall_flux(k,j,i) = -wall_flux(k,j,i) * us_wall |
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| 369 | |
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| 370 | ! |
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| 371 | !-- store rifs for next time step |
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| 372 | rif_wall(k,j,i,wall_index) = rifs |
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| 373 | |
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[1153] | 374 | ! ENDIF |
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[1015] | 375 | |
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[1153] | 376 | ENDDO |
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| 377 | |
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| 378 | ENDIF |
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| 379 | |
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[1015] | 380 | ENDDO |
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| 381 | ENDDO |
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| 382 | !$acc end kernels |
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| 383 | |
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| 384 | END SUBROUTINE wall_fluxes_acc |
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| 385 | |
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| 386 | |
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[56] | 387 | !------------------------------------------------------------------------------! |
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| 388 | ! Call for all grid point i,j |
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| 389 | !------------------------------------------------------------------------------! |
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| 390 | SUBROUTINE wall_fluxes_ij( i, j, nzb_w, nzt_w, wall_flux, a, b, c1, c2 ) |
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| 391 | |
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| 392 | USE arrays_3d |
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| 393 | USE control_parameters |
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| 394 | USE grid_variables |
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| 395 | USE indices |
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| 396 | USE statistics |
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| 397 | |
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| 398 | IMPLICIT NONE |
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| 399 | |
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| 400 | INTEGER :: i, j, k, nzb_w, nzt_w, wall_index |
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| 401 | REAL :: a, b, c1, c2, h1, h2, zp |
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| 402 | |
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| 403 | REAL :: pts, pt_i, rifs, u_i, v_i, us_wall, vel_total, ws, wspts |
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| 404 | |
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| 405 | REAL, DIMENSION(nzb:nzt+1) :: wall_flux |
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| 406 | |
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| 407 | |
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| 408 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 409 | wall_flux = 0.0 |
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| 410 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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| 411 | |
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| 412 | ! |
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| 413 | !-- All subsequent variables are computed for the respective location where |
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[187] | 414 | !-- the respective flux is defined. |
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[56] | 415 | DO k = nzb_w, nzt_w |
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| 416 | |
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| 417 | ! |
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| 418 | !-- (1) Compute rifs, u_i, v_i, ws, pt' and w'pt' |
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| 419 | rifs = rif_wall(k,j,i,wall_index) |
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| 420 | |
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| 421 | u_i = a * u(k,j,i) + c1 * 0.25 * & |
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| 422 | ( u(k+1,j,i+1) + u(k+1,j,i) + u(k,j,i+1) + u(k,j,i) ) |
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| 423 | |
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| 424 | v_i = b * v(k,j,i) + c2 * 0.25 * & |
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| 425 | ( v(k+1,j+1,i) + v(k+1,j,i) + v(k,j+1,i) + v(k,j,i) ) |
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| 426 | |
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| 427 | ws = ( c1 + c2 ) * w(k,j,i) + 0.25 * ( & |
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| 428 | a * ( w(k-1,j,i-1) + w(k-1,j,i) + w(k,j,i-1) + w(k,j,i) ) & |
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| 429 | + b * ( w(k-1,j-1,i) + w(k-1,j,i) + w(k,j-1,i) + w(k,j,i) ) & |
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| 430 | ) |
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| 431 | pt_i = 0.5 * ( pt(k,j,i) + a * pt(k,j,i-1) + b * pt(k,j-1,i) & |
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| 432 | + ( c1 + c2 ) * pt(k+1,j,i) ) |
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| 433 | |
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| 434 | pts = pt_i - hom(k,1,4,0) |
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| 435 | wspts = ws * pts |
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| 436 | |
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| 437 | ! |
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| 438 | !-- (2) Compute wall-parallel absolute velocity vel_total |
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| 439 | vel_total = SQRT( ws**2 + ( a+c1 ) * u_i**2 + ( b+c2 ) * v_i**2 ) |
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| 440 | |
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| 441 | ! |
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| 442 | !-- (3) Compute wall friction velocity us_wall |
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| 443 | IF ( rifs >= 0.0 ) THEN |
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| 444 | |
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| 445 | ! |
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| 446 | !-- Stable stratification (and neutral) |
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| 447 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 448 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 449 | ) |
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| 450 | ELSE |
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| 451 | |
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| 452 | ! |
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| 453 | !-- Unstable stratification |
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[187] | 454 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 455 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[56] | 456 | |
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[187] | 457 | us_wall = kappa * vel_total / ( & |
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| 458 | LOG( zp / z0(j,i) ) - & |
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| 459 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 460 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 461 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 462 | ) |
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[56] | 463 | ENDIF |
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| 464 | |
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| 465 | ! |
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| 466 | !-- (4) Compute zp/L (corresponds to neutral Richardson flux number |
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| 467 | !-- rifs) |
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| 468 | rifs = -1.0 * zp * kappa * g * wspts / ( pt_i * (us_wall**3 + 1E-30) ) |
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| 469 | |
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| 470 | ! |
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| 471 | !-- Limit the value range of the Richardson numbers. |
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| 472 | !-- This is necessary for very small velocities (u,w --> 0), because |
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| 473 | !-- the absolute value of rif can then become very large, which in |
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| 474 | !-- consequence would result in very large shear stresses and very |
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| 475 | !-- small momentum fluxes (both are generally unrealistic). |
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| 476 | IF ( rifs < rif_min ) rifs = rif_min |
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| 477 | IF ( rifs > rif_max ) rifs = rif_max |
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| 478 | |
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| 479 | ! |
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| 480 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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| 481 | IF ( rifs >= 0.0 ) THEN |
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| 482 | |
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| 483 | ! |
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| 484 | !-- Stable stratification (and neutral) |
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[53] | 485 | wall_flux(k) = kappa * & |
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| 486 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / & |
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[56] | 487 | ( LOG( zp / z0(j,i) ) + & |
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| 488 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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[53] | 489 | ) |
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[52] | 490 | ELSE |
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[53] | 491 | |
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[56] | 492 | ! |
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| 493 | !-- Unstable stratification |
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[187] | 494 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 495 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[52] | 496 | |
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[187] | 497 | wall_flux(k) = kappa * & |
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| 498 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / ( & |
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| 499 | LOG( zp / z0(j,i) ) - & |
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| 500 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 501 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 502 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 503 | ) |
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[56] | 504 | ENDIF |
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[187] | 505 | wall_flux(k) = -wall_flux(k) * us_wall |
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[53] | 506 | |
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[56] | 507 | ! |
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| 508 | !-- store rifs for next time step |
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| 509 | rif_wall(k,j,i,wall_index) = rifs |
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[53] | 510 | |
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[56] | 511 | ENDDO |
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[53] | 512 | |
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[56] | 513 | END SUBROUTINE wall_fluxes_ij |
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[53] | 514 | |
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[56] | 515 | |
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| 516 | |
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[53] | 517 | !------------------------------------------------------------------------------! |
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[56] | 518 | ! Call for all grid points |
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| 519 | !------------------------------------------------------------------------------! |
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| 520 | SUBROUTINE wall_fluxes_e( wall_flux, a, b, c1, c2, wall ) |
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| 521 | |
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| 522 | !------------------------------------------------------------------------------! |
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[53] | 523 | ! Description: |
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| 524 | ! ------------ |
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| 525 | ! Calculates momentum fluxes at vertical walls for routine production_e |
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| 526 | ! assuming Monin-Obukhov similarity. |
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| 527 | ! Indices: usvs a=1, vsus b=1, wsvs c1=1, wsus c2=1 (other=0). |
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| 528 | !------------------------------------------------------------------------------! |
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| 529 | |
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[56] | 530 | USE arrays_3d |
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| 531 | USE control_parameters |
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| 532 | USE grid_variables |
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| 533 | USE indices |
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| 534 | USE statistics |
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[53] | 535 | |
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[56] | 536 | IMPLICIT NONE |
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[53] | 537 | |
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[56] | 538 | INTEGER :: i, j, k, kk, wall_index |
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[187] | 539 | REAL :: a, b, c1, c2, h1, h2, u_i, v_i, us_wall, vel_total, vel_zp, & |
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| 540 | ws, zp |
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[53] | 541 | |
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[56] | 542 | REAL :: rifs |
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[53] | 543 | |
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[667] | 544 | REAL, DIMENSION(nysg:nyng,nxlg:nxrg) :: wall |
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[56] | 545 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
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[53] | 546 | |
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| 547 | |
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[56] | 548 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 549 | wall_flux = 0.0 |
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| 550 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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[53] | 551 | |
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[56] | 552 | DO i = nxl, nxr |
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| 553 | DO j = nys, nyn |
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| 554 | |
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| 555 | IF ( wall(j,i) /= 0.0 ) THEN |
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[53] | 556 | ! |
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[187] | 557 | !-- All subsequent variables are computed for scalar locations. |
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[56] | 558 | DO k = nzb_diff_s_inner(j,i)-1, nzb_diff_s_outer(j,i)-2 |
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[53] | 559 | ! |
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[187] | 560 | !-- (1) Compute rifs, u_i, v_i, and ws |
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[56] | 561 | IF ( k == nzb_diff_s_inner(j,i)-1 ) THEN |
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| 562 | kk = nzb_diff_s_inner(j,i)-1 |
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| 563 | ELSE |
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| 564 | kk = k-1 |
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| 565 | ENDIF |
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| 566 | rifs = 0.5 * ( rif_wall(k,j,i,wall_index) + & |
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| 567 | a * rif_wall(k,j,i+1,1) + b * rif_wall(k,j+1,i,2) + & |
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| 568 | c1 * rif_wall(kk,j,i,3) + c2 * rif_wall(kk,j,i,4) & |
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| 569 | ) |
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[53] | 570 | |
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[187] | 571 | u_i = 0.5 * ( u(k,j,i) + u(k,j,i+1) ) |
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| 572 | v_i = 0.5 * ( v(k,j,i) + v(k,j+1,i) ) |
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| 573 | ws = 0.5 * ( w(k,j,i) + w(k-1,j,i) ) |
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[53] | 574 | ! |
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[187] | 575 | !-- (2) Compute wall-parallel absolute velocity vel_total and |
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| 576 | !-- interpolate appropriate velocity component vel_zp. |
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| 577 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
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| 578 | vel_zp = 0.5 * ( a * u_i + b * v_i + (c1+c2) * ws ) |
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| 579 | ! |
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| 580 | !-- (3) Compute wall friction velocity us_wall |
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| 581 | IF ( rifs >= 0.0 ) THEN |
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[53] | 582 | |
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| 583 | ! |
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[187] | 584 | !-- Stable stratification (and neutral) |
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| 585 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 586 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 587 | ) |
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| 588 | ELSE |
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| 589 | |
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| 590 | ! |
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| 591 | !-- Unstable stratification |
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| 592 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 593 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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| 594 | |
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| 595 | us_wall = kappa * vel_total / ( & |
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| 596 | LOG( zp / z0(j,i) ) - & |
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| 597 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 598 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 599 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 600 | ) |
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| 601 | ENDIF |
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| 602 | |
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| 603 | ! |
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| 604 | !-- Skip step (4) of wall_fluxes, because here rifs is already |
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| 605 | !-- available from (1) |
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| 606 | ! |
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[56] | 607 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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[55] | 608 | |
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[56] | 609 | IF ( rifs >= 0.0 ) THEN |
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[53] | 610 | |
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| 611 | ! |
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[56] | 612 | !-- Stable stratification (and neutral) |
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| 613 | wall_flux(k,j,i) = kappa * vel_zp / & |
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| 614 | ( LOG( zp/z0(j,i) ) + 5.0*rifs * ( zp-z0(j,i) ) / zp ) |
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| 615 | ELSE |
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[53] | 616 | |
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| 617 | ! |
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[56] | 618 | !-- Unstable stratification |
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[187] | 619 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 620 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[53] | 621 | |
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[187] | 622 | wall_flux(k,j,i) = kappa * vel_zp / ( & |
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| 623 | LOG( zp / z0(j,i) ) - & |
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| 624 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 625 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 626 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 627 | ) |
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[56] | 628 | ENDIF |
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[187] | 629 | wall_flux(k,j,i) = - wall_flux(k,j,i) * us_wall |
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[56] | 630 | |
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| 631 | ENDDO |
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| 632 | |
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| 633 | ENDIF |
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| 634 | |
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| 635 | ENDDO |
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| 636 | ENDDO |
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| 637 | |
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| 638 | END SUBROUTINE wall_fluxes_e |
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| 639 | |
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| 640 | |
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[1015] | 641 | !------------------------------------------------------------------------------! |
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| 642 | ! Call for all grid points - accelerator version |
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| 643 | !------------------------------------------------------------------------------! |
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| 644 | SUBROUTINE wall_fluxes_e_acc( wall_flux, a, b, c1, c2, wall ) |
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[56] | 645 | |
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| 646 | !------------------------------------------------------------------------------! |
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[1015] | 647 | ! Description: |
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| 648 | ! ------------ |
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| 649 | ! Calculates momentum fluxes at vertical walls for routine production_e |
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| 650 | ! assuming Monin-Obukhov similarity. |
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| 651 | ! Indices: usvs a=1, vsus b=1, wsvs c1=1, wsus c2=1 (other=0). |
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| 652 | !------------------------------------------------------------------------------! |
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| 653 | |
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| 654 | USE arrays_3d |
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| 655 | USE control_parameters |
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| 656 | USE grid_variables |
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| 657 | USE indices |
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| 658 | USE statistics |
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| 659 | |
---|
| 660 | IMPLICIT NONE |
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| 661 | |
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| 662 | INTEGER :: i, j, k, kk, max_outer, min_inner, wall_index |
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| 663 | REAL :: a, b, c1, c2, h1, h2, u_i, v_i, us_wall, vel_total, vel_zp, & |
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| 664 | ws, zp |
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| 665 | |
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| 666 | REAL :: rifs |
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| 667 | |
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| 668 | REAL, DIMENSION(nysg:nyng,nxlg:nxrg) :: wall |
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| 669 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
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| 670 | |
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| 671 | |
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| 672 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 673 | wall_flux = 0.0 |
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| 674 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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| 675 | |
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| 676 | min_inner = MINVAL( nzb_diff_s_inner(nys:nyn,nxl:nxr) ) - 1 |
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| 677 | max_outer = MAXVAL( nzb_diff_s_outer(nys:nyn,nxl:nxr) ) - 2 |
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| 678 | |
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| 679 | !$acc kernels present( nzb_diff_s_inner, nzb_diff_s_outer, pt, rif_wall ) & |
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| 680 | !$acc present( u, v, w, wall, wall_flux, z0 ) |
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[1128] | 681 | DO i = i_left, i_right |
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| 682 | DO j = j_south, j_north |
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[1015] | 683 | DO k = min_inner, max_outer |
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| 684 | ! |
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| 685 | !-- All subsequent variables are computed for scalar locations |
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| 686 | IF ( k >= nzb_diff_s_inner(j,i)-1 .AND. & |
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| 687 | k <= nzb_diff_s_outer(j,i)-2 .AND. wall(j,i) /= 0.0 ) THEN |
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| 688 | ! |
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| 689 | !-- (1) Compute rifs, u_i, v_i, and ws |
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| 690 | IF ( k == nzb_diff_s_inner(j,i)-1 ) THEN |
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| 691 | kk = nzb_diff_s_inner(j,i)-1 |
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| 692 | ELSE |
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| 693 | kk = k-1 |
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| 694 | ENDIF |
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| 695 | rifs = 0.5 * ( rif_wall(k,j,i,wall_index) + & |
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| 696 | a * rif_wall(k,j,i+1,1) + b * rif_wall(k,j+1,i,2) + & |
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| 697 | c1 * rif_wall(kk,j,i,3) + c2 * rif_wall(kk,j,i,4) & |
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| 698 | ) |
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| 699 | |
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| 700 | u_i = 0.5 * ( u(k,j,i) + u(k,j,i+1) ) |
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| 701 | v_i = 0.5 * ( v(k,j,i) + v(k,j+1,i) ) |
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| 702 | ws = 0.5 * ( w(k,j,i) + w(k-1,j,i) ) |
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| 703 | ! |
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| 704 | !-- (2) Compute wall-parallel absolute velocity vel_total and |
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| 705 | !-- interpolate appropriate velocity component vel_zp. |
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| 706 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
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| 707 | vel_zp = 0.5 * ( a * u_i + b * v_i + (c1+c2) * ws ) |
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| 708 | ! |
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| 709 | !-- (3) Compute wall friction velocity us_wall |
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| 710 | IF ( rifs >= 0.0 ) THEN |
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| 711 | |
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| 712 | ! |
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| 713 | !-- Stable stratification (and neutral) |
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| 714 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 715 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 716 | ) |
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| 717 | ELSE |
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| 718 | |
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| 719 | ! |
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| 720 | !-- Unstable stratification |
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| 721 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 722 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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| 723 | |
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| 724 | us_wall = kappa * vel_total / ( & |
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| 725 | LOG( zp / z0(j,i) ) - & |
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| 726 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 727 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 728 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 729 | ) |
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| 730 | ENDIF |
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| 731 | |
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| 732 | ! |
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| 733 | !-- Skip step (4) of wall_fluxes, because here rifs is already |
---|
| 734 | !-- available from (1) |
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| 735 | ! |
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| 736 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
---|
| 737 | |
---|
| 738 | IF ( rifs >= 0.0 ) THEN |
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| 739 | |
---|
| 740 | ! |
---|
| 741 | !-- Stable stratification (and neutral) |
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| 742 | wall_flux(k,j,i) = kappa * vel_zp / & |
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| 743 | ( LOG( zp/z0(j,i) ) + 5.0*rifs * ( zp-z0(j,i) ) / zp ) |
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| 744 | ELSE |
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| 745 | |
---|
| 746 | ! |
---|
| 747 | !-- Unstable stratification |
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| 748 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
| 749 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
| 750 | |
---|
| 751 | wall_flux(k,j,i) = kappa * vel_zp / ( & |
---|
| 752 | LOG( zp / z0(j,i) ) - & |
---|
| 753 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
| 754 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
| 755 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
| 756 | ) |
---|
| 757 | ENDIF |
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| 758 | wall_flux(k,j,i) = - wall_flux(k,j,i) * us_wall |
---|
| 759 | |
---|
| 760 | ENDIF |
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| 761 | |
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| 762 | ENDDO |
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| 763 | ENDDO |
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| 764 | ENDDO |
---|
| 765 | !$acc end kernels |
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| 766 | |
---|
| 767 | END SUBROUTINE wall_fluxes_e_acc |
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| 768 | |
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| 769 | |
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| 770 | !------------------------------------------------------------------------------! |
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[56] | 771 | ! Call for grid point i,j |
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| 772 | !------------------------------------------------------------------------------! |
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| 773 | SUBROUTINE wall_fluxes_e_ij( i, j, nzb_w, nzt_w, wall_flux, a, b, c1, c2 ) |
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| 774 | |
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| 775 | USE arrays_3d |
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| 776 | USE control_parameters |
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| 777 | USE grid_variables |
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| 778 | USE indices |
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| 779 | USE statistics |
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| 780 | |
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| 781 | IMPLICIT NONE |
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| 782 | |
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| 783 | INTEGER :: i, j, k, kk, nzb_w, nzt_w, wall_index |
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[187] | 784 | REAL :: a, b, c1, c2, h1, h2, u_i, v_i, us_wall, vel_total, vel_zp, & |
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| 785 | ws, zp |
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[56] | 786 | |
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| 787 | REAL :: rifs |
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| 788 | |
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| 789 | REAL, DIMENSION(nzb:nzt+1) :: wall_flux |
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| 790 | |
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| 791 | |
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| 792 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 793 | wall_flux = 0.0 |
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| 794 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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| 795 | |
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| 796 | ! |
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[187] | 797 | !-- All subsequent variables are computed for scalar locations. |
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[56] | 798 | DO k = nzb_w, nzt_w |
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| 799 | |
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| 800 | ! |
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[187] | 801 | !-- (1) Compute rifs, u_i, v_i, and ws |
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[56] | 802 | IF ( k == nzb_w ) THEN |
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| 803 | kk = nzb_w |
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[53] | 804 | ELSE |
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[56] | 805 | kk = k-1 |
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| 806 | ENDIF |
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| 807 | rifs = 0.5 * ( rif_wall(k,j,i,wall_index) + & |
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| 808 | a * rif_wall(k,j,i+1,1) + b * rif_wall(k,j+1,i,2) + & |
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| 809 | c1 * rif_wall(kk,j,i,3) + c2 * rif_wall(kk,j,i,4) & |
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| 810 | ) |
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| 811 | |
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[187] | 812 | u_i = 0.5 * ( u(k,j,i) + u(k,j,i+1) ) |
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| 813 | v_i = 0.5 * ( v(k,j,i) + v(k,j+1,i) ) |
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| 814 | ws = 0.5 * ( w(k,j,i) + w(k-1,j,i) ) |
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[56] | 815 | ! |
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[187] | 816 | !-- (2) Compute wall-parallel absolute velocity vel_total and |
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| 817 | !-- interpolate appropriate velocity component vel_zp. |
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| 818 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
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| 819 | vel_zp = 0.5 * ( a * u_i + b * v_i + (c1+c2) * ws ) |
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| 820 | ! |
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| 821 | !-- (3) Compute wall friction velocity us_wall |
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| 822 | IF ( rifs >= 0.0 ) THEN |
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[56] | 823 | |
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| 824 | ! |
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[187] | 825 | !-- Stable stratification (and neutral) |
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| 826 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 827 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 828 | ) |
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| 829 | ELSE |
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| 830 | |
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| 831 | ! |
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| 832 | !-- Unstable stratification |
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| 833 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 834 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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| 835 | |
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| 836 | us_wall = kappa * vel_total / ( & |
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| 837 | LOG( zp / z0(j,i) ) - & |
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| 838 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 839 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 840 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 841 | ) |
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| 842 | ENDIF |
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| 843 | |
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| 844 | ! |
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| 845 | !-- Skip step (4) of wall_fluxes, because here rifs is already |
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| 846 | !-- available from (1) |
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| 847 | ! |
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[56] | 848 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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[187] | 849 | !-- First interpolate the velocity (this is different from |
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| 850 | !-- subroutine wall_fluxes because fluxes in subroutine |
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| 851 | !-- wall_fluxes_e are defined at scalar locations). |
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[56] | 852 | vel_zp = 0.5 * ( a * ( u(k,j,i) + u(k,j,i+1) ) + & |
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| 853 | b * ( v(k,j,i) + v(k,j+1,i) ) + & |
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| 854 | (c1+c2) * ( w(k,j,i) + w(k-1,j,i) ) & |
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| 855 | ) |
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| 856 | |
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| 857 | IF ( rifs >= 0.0 ) THEN |
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| 858 | |
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| 859 | ! |
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| 860 | !-- Stable stratification (and neutral) |
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| 861 | wall_flux(k) = kappa * vel_zp / & |
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| 862 | ( LOG( zp/z0(j,i) ) + 5.0*rifs * ( zp-z0(j,i) ) / zp ) |
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| 863 | ELSE |
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| 864 | |
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| 865 | ! |
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| 866 | !-- Unstable stratification |
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[187] | 867 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 868 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[56] | 869 | |
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[187] | 870 | wall_flux(k) = kappa * vel_zp / ( & |
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| 871 | LOG( zp / z0(j,i) ) - & |
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| 872 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 873 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 874 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 875 | ) |
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[53] | 876 | ENDIF |
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[187] | 877 | wall_flux(k) = - wall_flux(k) * us_wall |
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[53] | 878 | |
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[56] | 879 | ENDDO |
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[53] | 880 | |
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[56] | 881 | END SUBROUTINE wall_fluxes_e_ij |
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| 882 | |
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| 883 | END MODULE wall_fluxes_mod |
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