| [1] | 1 | SUBROUTINE prandtl_fluxes |
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| 2 | |
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| [1036] | 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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| 17 | ! Copyright 1997-2012 Leibniz University Hannover |
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| 18 | !--------------------------------------------------------------------------------! |
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| 19 | ! |
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| [484] | 20 | ! Current revisions: |
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| [1] | 21 | ! ----------------- |
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| [1276] | 22 | ! Use LSF_DATA also in case of Dirichlet bottom boundary condition for scalars |
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| [1] | 23 | ! |
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| [668] | 24 | ! Former revisions: |
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| 25 | ! ----------------- |
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| 26 | ! $Id: prandtl_fluxes.f90 1276 2014-01-15 13:40:41Z 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 "kernels do" replaced by "kernels loop", "loop independent" added |
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| 30 | ! |
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| [1037] | 31 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 32 | ! code put under GPL (PALM 3.9) |
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| 33 | ! |
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| [1017] | 34 | ! 1015 2012-09-27 09:23:24Z raasch |
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| 35 | ! OpenACC statements added |
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| 36 | ! |
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| [979] | 37 | ! 978 2012-08-09 08:28:32Z fricke |
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| 38 | ! roughness length for scalar quantities z0h added |
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| 39 | ! |
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| [760] | 40 | ! 759 2011-09-15 13:58:31Z raasch |
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| 41 | ! Bugfix for ts limitation |
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| 42 | ! |
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| [710] | 43 | ! 709 2011-03-30 09:31:40Z raasch |
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| 44 | ! formatting adjustments |
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| 45 | ! |
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| [668] | 46 | ! 667 2010-12-23 12:06:00Z suehring/gryschka |
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| [709] | 47 | ! Changed surface boundary conditions for u and v from mirror to Dirichlet. |
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| 48 | ! Therefore u(uzb,:,:) and v(nzb,:,:) are now representative for height z0. |
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| [667] | 49 | ! nxl-1, nxr+1, nys-1, nyn+1 replaced by nxlg, nxrg, nysg, nyng |
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| 50 | ! |
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| [392] | 51 | ! 315 2009-05-13 10:57:59Z raasch |
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| 52 | ! Saturation condition at (sea) surface is not used in precursor runs (only |
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| 53 | ! in the following coupled runs) |
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| 54 | ! Bugfix: qsws was calculated in case of constant heatflux = .FALSE. |
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| 55 | ! |
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| [198] | 56 | ! 187 2008-08-06 16:25:09Z letzel |
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| 57 | ! Bugfix: modification of the calculation of the vertical turbulent momentum |
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| 58 | ! fluxes u'w' and v'w' |
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| 59 | ! Bugfix: change definition of us_wall from 1D to 2D |
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| 60 | ! Change: modification of the integrated version of the profile function for |
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| 61 | ! momentum for unstable stratification (does not effect results) |
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| 62 | ! |
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| [110] | 63 | ! 108 2007-08-24 15:10:38Z letzel |
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| 64 | ! assume saturation at k=nzb_s_inner(j,i) for atmosphere coupled to ocean |
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| 65 | ! |
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| [77] | 66 | ! 75 2007-03-22 09:54:05Z raasch |
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| 67 | ! moisture renamed humidity |
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| 68 | ! |
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| [3] | 69 | ! RCS Log replace by Id keyword, revision history cleaned up |
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| 70 | ! |
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| [1] | 71 | ! Revision 1.19 2006/04/26 12:24:35 raasch |
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| 72 | ! +OpenMP directives and optimization (array assignments replaced by DO loops) |
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| 73 | ! |
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| 74 | ! Revision 1.1 1998/01/23 10:06:06 raasch |
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| 75 | ! Initial revision |
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| 76 | ! |
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| 77 | ! |
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| 78 | ! Description: |
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| 79 | ! ------------ |
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| 80 | ! Diagnostic computation of vertical fluxes in the Prandtl layer from the |
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| 81 | ! values of the variables at grid point k=1 |
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| 82 | !------------------------------------------------------------------------------! |
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| 83 | |
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| 84 | USE arrays_3d |
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| 85 | USE control_parameters |
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| 86 | USE grid_variables |
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| 87 | USE indices |
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| 88 | |
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| 89 | IMPLICIT NONE |
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| 90 | |
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| 91 | INTEGER :: i, j, k |
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| [1015] | 92 | LOGICAL :: coupled_run |
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| [108] | 93 | REAL :: a, b, e_q, rifm, uv_total, z_p |
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| [1] | 94 | |
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| [1015] | 95 | ! |
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| 96 | !-- Data information for accelerators |
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| 97 | !$acc data present( e, nzb_u_inner, nzb_v_inner, nzb_s_inner, pt, q, qs ) & |
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| 98 | !$acc present( qsws, rif, shf, ts, u, us, usws, v, vpt, vsws, zu, zw, z0, z0h ) |
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| [667] | 99 | ! |
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| [1] | 100 | !-- Compute theta* |
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| 101 | IF ( constant_heatflux ) THEN |
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| 102 | ! |
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| 103 | !-- For a given heat flux in the Prandtl layer: |
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| 104 | !-- for u* use the value from the previous time step |
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| 105 | !$OMP PARALLEL DO |
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| [1257] | 106 | !$acc kernels loop |
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| [667] | 107 | DO i = nxlg, nxrg |
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| 108 | DO j = nysg, nyng |
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| [1] | 109 | ts(j,i) = -shf(j,i) / ( us(j,i) + 1E-30 ) |
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| 110 | ! |
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| 111 | !-- ts must be limited, because otherwise overflow may occur in case of |
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| 112 | !-- us=0 when computing rif further below |
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| [759] | 113 | IF ( ts(j,i) < -1.05E5 ) ts(j,i) = -1.0E5 |
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| 114 | IF ( ts(j,i) > 1.0E5 ) ts(j,i) = 1.0E5 |
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| [1] | 115 | ENDDO |
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| 116 | ENDDO |
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| 117 | |
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| 118 | ELSE |
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| 119 | ! |
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| 120 | !-- For a given surface temperature: |
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| 121 | !-- (the Richardson number is still the one from the previous time step) |
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| [1276] | 122 | |
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| 123 | IF ( large_scale_forcing .AND. lsf_surf ) THEN |
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| 124 | pt(0,:,:) = pt_surface |
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| 125 | ENDIF |
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| 126 | |
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| [1] | 127 | !$OMP PARALLEL DO PRIVATE( a, b, k, z_p ) |
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| [1257] | 128 | !$acc kernels loop |
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| [667] | 129 | DO i = nxlg, nxrg |
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| 130 | DO j = nysg, nyng |
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| [1] | 131 | |
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| 132 | k = nzb_s_inner(j,i) |
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| 133 | z_p = zu(k+1) - zw(k) |
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| 134 | |
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| 135 | IF ( rif(j,i) >= 0.0 ) THEN |
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| 136 | ! |
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| 137 | !-- Stable stratification |
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| [978] | 138 | ts(j,i) = kappa * ( pt(k+1,j,i) - pt(k,j,i) ) / ( & |
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| 139 | LOG( z_p / z0h(j,i) ) + & |
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| 140 | 5.0 * rif(j,i) * ( z_p - z0h(j,i) ) / z_p & |
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| [1] | 141 | ) |
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| 142 | ELSE |
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| 143 | ! |
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| 144 | !-- Unstable stratification |
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| 145 | a = SQRT( 1.0 - 16.0 * rif(j,i) ) |
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| [978] | 146 | b = SQRT( 1.0 - 16.0 * rif(j,i) * z0h(j,i) / z_p ) |
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| [187] | 147 | |
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| [978] | 148 | ts(j,i) = kappa * ( pt(k+1,j,i) - pt(k,j,i) ) / ( & |
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| 149 | LOG( z_p / z0h(j,i) ) - & |
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| [187] | 150 | 2.0 * LOG( ( 1.0 + a ) / ( 1.0 + b ) ) ) |
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| [1] | 151 | ENDIF |
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| 152 | |
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| 153 | ENDDO |
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| 154 | ENDDO |
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| 155 | ENDIF |
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| 156 | |
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| 157 | ! |
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| 158 | !-- Compute z_p/L (corresponds to the Richardson-flux number) |
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| [75] | 159 | IF ( .NOT. humidity ) THEN |
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| [1] | 160 | !$OMP PARALLEL DO PRIVATE( k, z_p ) |
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| [1257] | 161 | !$acc kernels loop |
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| [667] | 162 | DO i = nxlg, nxrg |
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| 163 | DO j = nysg, nyng |
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| [1] | 164 | k = nzb_s_inner(j,i) |
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| 165 | z_p = zu(k+1) - zw(k) |
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| 166 | rif(j,i) = z_p * kappa * g * ts(j,i) / & |
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| 167 | ( pt(k+1,j,i) * ( us(j,i)**2 + 1E-30 ) ) |
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| 168 | ! |
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| 169 | !-- Limit the value range of the Richardson numbers. |
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| 170 | !-- This is necessary for very small velocities (u,v --> 0), because |
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| 171 | !-- the absolute value of rif can then become very large, which in |
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| 172 | !-- consequence would result in very large shear stresses and very |
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| 173 | !-- small momentum fluxes (both are generally unrealistic). |
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| 174 | IF ( rif(j,i) < rif_min ) rif(j,i) = rif_min |
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| 175 | IF ( rif(j,i) > rif_max ) rif(j,i) = rif_max |
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| 176 | ENDDO |
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| 177 | ENDDO |
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| 178 | ELSE |
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| 179 | !$OMP PARALLEL DO PRIVATE( k, z_p ) |
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| [1257] | 180 | !$acc kernels loop |
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| [667] | 181 | DO i = nxlg, nxrg |
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| 182 | DO j = nysg, nyng |
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| [1] | 183 | k = nzb_s_inner(j,i) |
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| 184 | z_p = zu(k+1) - zw(k) |
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| 185 | rif(j,i) = z_p * kappa * g * & |
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| 186 | ( ts(j,i) + 0.61 * pt(k+1,j,i) * qs(j,i) ) / & |
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| 187 | ( vpt(k+1,j,i) * ( us(j,i)**2 + 1E-30 ) ) |
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| 188 | ! |
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| 189 | !-- Limit the value range of the Richardson numbers. |
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| 190 | !-- This is necessary for very small velocities (u,v --> 0), because |
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| 191 | !-- the absolute value of rif can then become very large, which in |
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| 192 | !-- consequence would result in very large shear stresses and very |
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| 193 | !-- small momentum fluxes (both are generally unrealistic). |
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| 194 | IF ( rif(j,i) < rif_min ) rif(j,i) = rif_min |
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| 195 | IF ( rif(j,i) > rif_max ) rif(j,i) = rif_max |
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| 196 | ENDDO |
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| 197 | ENDDO |
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| 198 | ENDIF |
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| 199 | |
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| 200 | ! |
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| 201 | !-- Compute u* at the scalars' grid points |
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| 202 | !$OMP PARALLEL DO PRIVATE( a, b, k, uv_total, z_p ) |
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| [1257] | 203 | !$acc kernels loop |
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| [1] | 204 | DO i = nxl, nxr |
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| 205 | DO j = nys, nyn |
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| 206 | |
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| 207 | k = nzb_s_inner(j,i) |
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| 208 | z_p = zu(k+1) - zw(k) |
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| 209 | |
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| 210 | ! |
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| [667] | 211 | !-- Compute the absolute value of the horizontal velocity |
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| 212 | !-- (relative to the surface) |
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| 213 | uv_total = SQRT( ( 0.5 * ( u(k+1,j,i) + u(k+1,j,i+1) & |
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| 214 | - u(k,j,i) - u(k,j,i+1) ) )**2 + & |
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| 215 | ( 0.5 * ( v(k+1,j,i) + v(k+1,j+1,i) & |
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| 216 | - v(k,j,i) - v(k,j+1,i) ) )**2 ) |
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| [1] | 217 | |
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| [667] | 218 | |
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| [1] | 219 | IF ( rif(j,i) >= 0.0 ) THEN |
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| 220 | ! |
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| 221 | !-- Stable stratification |
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| 222 | us(j,i) = kappa * uv_total / ( & |
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| 223 | LOG( z_p / z0(j,i) ) + & |
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| 224 | 5.0 * rif(j,i) * ( z_p - z0(j,i) ) / z_p & |
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| 225 | ) |
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| 226 | ELSE |
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| 227 | ! |
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| 228 | !-- Unstable stratification |
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| [187] | 229 | a = SQRT( SQRT( 1.0 - 16.0 * rif(j,i) ) ) |
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| 230 | b = SQRT( SQRT( 1.0 - 16.0 * rif(j,i) / z_p * z0(j,i) ) ) |
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| 231 | |
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| 232 | us(j,i) = kappa * uv_total / ( & |
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| 233 | LOG( z_p / z0(j,i) ) - & |
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| 234 | LOG( ( 1.0 + a )**2 * ( 1.0 + a**2 ) / ( & |
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| 235 | ( 1.0 + b )**2 * ( 1.0 + b**2 ) ) ) + & |
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| 236 | 2.0 * ( ATAN( a ) - ATAN( b ) ) & |
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| 237 | ) |
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| [1] | 238 | ENDIF |
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| 239 | ENDDO |
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| 240 | ENDDO |
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| 241 | |
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| 242 | ! |
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| [187] | 243 | !-- Values of us at ghost point locations are needed for the evaluation of usws |
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| 244 | !-- and vsws. |
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| [1015] | 245 | !$acc update host( us ) |
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| [187] | 246 | CALL exchange_horiz_2d( us ) |
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| [1015] | 247 | !$acc update device( us ) |
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| 248 | |
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| [187] | 249 | ! |
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| [1] | 250 | !-- Compute u'w' for the total model domain. |
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| 251 | !-- First compute the corresponding component of u* and square it. |
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| 252 | !$OMP PARALLEL DO PRIVATE( a, b, k, rifm, z_p ) |
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| [1257] | 253 | !$acc kernels loop |
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| [1] | 254 | DO i = nxl, nxr |
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| 255 | DO j = nys, nyn |
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| 256 | |
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| 257 | k = nzb_u_inner(j,i) |
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| 258 | z_p = zu(k+1) - zw(k) |
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| 259 | |
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| 260 | ! |
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| 261 | !-- Compute Richardson-flux number for this point |
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| 262 | rifm = 0.5 * ( rif(j,i-1) + rif(j,i) ) |
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| 263 | IF ( rifm >= 0.0 ) THEN |
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| 264 | ! |
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| 265 | !-- Stable stratification |
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| [667] | 266 | usws(j,i) = kappa * ( u(k+1,j,i) - u(k,j,i) )/ ( & |
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| [1] | 267 | LOG( z_p / z0(j,i) ) + & |
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| 268 | 5.0 * rifm * ( z_p - z0(j,i) ) / z_p & |
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| 269 | ) |
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| 270 | ELSE |
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| 271 | ! |
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| 272 | !-- Unstable stratification |
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| [187] | 273 | a = SQRT( SQRT( 1.0 - 16.0 * rifm ) ) |
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| 274 | b = SQRT( SQRT( 1.0 - 16.0 * rifm / z_p * z0(j,i) ) ) |
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| 275 | |
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| [667] | 276 | usws(j,i) = kappa * ( u(k+1,j,i) - u(k,j,i) ) / ( & |
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| [187] | 277 | LOG( z_p / z0(j,i) ) - & |
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| 278 | LOG( (1.0 + a )**2 * ( 1.0 + a**2 ) / ( & |
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| 279 | (1.0 + b )**2 * ( 1.0 + b**2 ) ) ) + & |
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| 280 | 2.0 * ( ATAN( a ) - ATAN( b ) ) & |
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| [1] | 281 | ) |
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| 282 | ENDIF |
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| [187] | 283 | usws(j,i) = -usws(j,i) * 0.5 * ( us(j,i-1) + us(j,i) ) |
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| [1] | 284 | ENDDO |
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| 285 | ENDDO |
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| 286 | |
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| 287 | ! |
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| 288 | !-- Compute v'w' for the total model domain. |
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| 289 | !-- First compute the corresponding component of u* and square it. |
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| 290 | !$OMP PARALLEL DO PRIVATE( a, b, k, rifm, z_p ) |
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| [1257] | 291 | !$acc kernels loop |
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| [1] | 292 | DO i = nxl, nxr |
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| 293 | DO j = nys, nyn |
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| 294 | |
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| 295 | k = nzb_v_inner(j,i) |
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| 296 | z_p = zu(k+1) - zw(k) |
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| 297 | |
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| 298 | ! |
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| 299 | !-- Compute Richardson-flux number for this point |
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| 300 | rifm = 0.5 * ( rif(j-1,i) + rif(j,i) ) |
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| 301 | IF ( rifm >= 0.0 ) THEN |
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| 302 | ! |
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| 303 | !-- Stable stratification |
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| [667] | 304 | vsws(j,i) = kappa * ( v(k+1,j,i) - v(k,j,i) ) / ( & |
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| [1] | 305 | LOG( z_p / z0(j,i) ) + & |
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| 306 | 5.0 * rifm * ( z_p - z0(j,i) ) / z_p & |
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| 307 | ) |
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| 308 | ELSE |
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| 309 | ! |
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| 310 | !-- Unstable stratification |
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| [187] | 311 | a = SQRT( SQRT( 1.0 - 16.0 * rifm ) ) |
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| 312 | b = SQRT( SQRT( 1.0 - 16.0 * rifm / z_p * z0(j,i) ) ) |
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| 313 | |
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| [667] | 314 | vsws(j,i) = kappa * ( v(k+1,j,i) - v(k,j,i) ) / ( & |
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| [187] | 315 | LOG( z_p / z0(j,i) ) - & |
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| 316 | LOG( (1.0 + a )**2 * ( 1.0 + a**2 ) / ( & |
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| 317 | (1.0 + b )**2 * ( 1.0 + b**2 ) ) ) + & |
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| 318 | 2.0 * ( ATAN( a ) - ATAN( b ) ) & |
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| [1] | 319 | ) |
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| 320 | ENDIF |
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| [187] | 321 | vsws(j,i) = -vsws(j,i) * 0.5 * ( us(j-1,i) + us(j,i) ) |
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| [1] | 322 | ENDDO |
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| 323 | ENDDO |
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| 324 | |
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| 325 | ! |
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| 326 | !-- If required compute q* |
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| [75] | 327 | IF ( humidity .OR. passive_scalar ) THEN |
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| [1] | 328 | IF ( constant_waterflux ) THEN |
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| 329 | ! |
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| 330 | !-- For a given water flux in the Prandtl layer: |
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| 331 | !$OMP PARALLEL DO |
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| [1257] | 332 | !$acc kernels loop |
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| [667] | 333 | DO i = nxlg, nxrg |
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| 334 | DO j = nysg, nyng |
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| [1] | 335 | qs(j,i) = -qsws(j,i) / ( us(j,i) + 1E-30 ) |
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| 336 | ENDDO |
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| 337 | ENDDO |
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| 338 | |
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| [1015] | 339 | ELSE |
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| 340 | coupled_run = ( coupling_mode == 'atmosphere_to_ocean' .AND. run_coupled ) |
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| [1276] | 341 | |
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| 342 | IF ( large_scale_forcing .AND. lsf_surf ) THEN |
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| 343 | q(0,:,:) = q_surface |
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| 344 | ENDIF |
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| 345 | |
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| [1] | 346 | !$OMP PARALLEL DO PRIVATE( a, b, k, z_p ) |
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| [1257] | 347 | !$acc kernels loop independent |
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| [667] | 348 | DO i = nxlg, nxrg |
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| [1257] | 349 | !$acc loop independent |
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| [667] | 350 | DO j = nysg, nyng |
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| [1] | 351 | |
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| 352 | k = nzb_s_inner(j,i) |
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| 353 | z_p = zu(k+1) - zw(k) |
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| 354 | |
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| [108] | 355 | ! |
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| [291] | 356 | !-- Assume saturation for atmosphere coupled to ocean (but not |
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| 357 | !-- in case of precursor runs) |
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| [1015] | 358 | IF ( coupled_run ) THEN |
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| [108] | 359 | e_q = 6.1 * & |
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| 360 | EXP( 0.07 * ( MIN(pt(0,j,i),pt(1,j,i)) - 273.15 ) ) |
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| 361 | q(k,j,i) = 0.622 * e_q / ( surface_pressure - e_q ) |
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| 362 | ENDIF |
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| [1] | 363 | IF ( rif(j,i) >= 0.0 ) THEN |
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| 364 | ! |
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| 365 | !-- Stable stratification |
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| [978] | 366 | qs(j,i) = kappa * ( q(k+1,j,i) - q(k,j,i) ) / ( & |
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| 367 | LOG( z_p / z0h(j,i) ) + & |
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| 368 | 5.0 * rif(j,i) * ( z_p - z0h(j,i) ) / z_p & |
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| [1] | 369 | ) |
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| 370 | ELSE |
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| 371 | ! |
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| 372 | !-- Unstable stratification |
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| [187] | 373 | a = SQRT( 1.0 - 16.0 * rif(j,i) ) |
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| [978] | 374 | b = SQRT( 1.0 - 16.0 * rif(j,i) * z0h(j,i) / z_p ) |
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| [187] | 375 | |
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| [978] | 376 | qs(j,i) = kappa * ( q(k+1,j,i) - q(k,j,i) ) / ( & |
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| 377 | LOG( z_p / z0h(j,i) ) - & |
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| [187] | 378 | 2.0 * LOG( (1.0 + a ) / ( 1.0 + b ) ) ) |
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| [1] | 379 | ENDIF |
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| 380 | |
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| 381 | ENDDO |
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| 382 | ENDDO |
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| 383 | ENDIF |
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| 384 | ENDIF |
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| 385 | |
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| 386 | ! |
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| [187] | 387 | !-- Exchange the boundaries for the momentum fluxes (only for sake of |
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| 388 | !-- completeness) |
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| [1015] | 389 | !$acc update host( usws, vsws ) |
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| [1] | 390 | CALL exchange_horiz_2d( usws ) |
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| 391 | CALL exchange_horiz_2d( vsws ) |
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| [1015] | 392 | !$acc update device( usws, vsws ) |
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| 393 | IF ( humidity .OR. passive_scalar ) THEN |
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| 394 | !$acc update host( qsws ) |
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| 395 | CALL exchange_horiz_2d( qsws ) |
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| 396 | !$acc update device( qsws ) |
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| 397 | ENDIF |
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| [1] | 398 | |
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| 399 | ! |
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| 400 | !-- Compute the vertical kinematic heat flux |
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| 401 | IF ( .NOT. constant_heatflux ) THEN |
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| 402 | !$OMP PARALLEL DO |
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| [1257] | 403 | !$acc kernels loop independent |
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| [667] | 404 | DO i = nxlg, nxrg |
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| [1257] | 405 | !$acc loop independent |
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| [667] | 406 | DO j = nysg, nyng |
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| [1] | 407 | shf(j,i) = -ts(j,i) * us(j,i) |
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| 408 | ENDDO |
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| 409 | ENDDO |
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| 410 | ENDIF |
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| 411 | |
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| 412 | ! |
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| 413 | !-- Compute the vertical water/scalar flux |
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| [315] | 414 | IF ( .NOT. constant_waterflux .AND. ( humidity .OR. passive_scalar ) ) THEN |
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| [1] | 415 | !$OMP PARALLEL DO |
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| [1257] | 416 | !$acc kernels loop independent |
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| [667] | 417 | DO i = nxlg, nxrg |
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| [1257] | 418 | !$acc loop independent |
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| [667] | 419 | DO j = nysg, nyng |
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| [1] | 420 | qsws(j,i) = -qs(j,i) * us(j,i) |
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| 421 | ENDDO |
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| 422 | ENDDO |
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| 423 | ENDIF |
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| 424 | |
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| 425 | ! |
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| 426 | !-- Bottom boundary condition for the TKE |
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| 427 | IF ( ibc_e_b == 2 ) THEN |
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| 428 | !$OMP PARALLEL DO |
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| [1257] | 429 | !$acc kernels loop independent |
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| [667] | 430 | DO i = nxlg, nxrg |
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| [1257] | 431 | !$acc loop independent |
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| [667] | 432 | DO j = nysg, nyng |
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| [1] | 433 | e(nzb_s_inner(j,i)+1,j,i) = ( us(j,i) / 0.1 )**2 |
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| 434 | ! |
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| 435 | !-- As a test: cm = 0.4 |
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| 436 | ! e(nzb_s_inner(j,i)+1,j,i) = ( us(j,i) / 0.4 )**2 |
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| 437 | e(nzb_s_inner(j,i),j,i) = e(nzb_s_inner(j,i)+1,j,i) |
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| 438 | ENDDO |
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| 439 | ENDDO |
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| 440 | ENDIF |
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| 441 | |
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| [1015] | 442 | !$acc end data |
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| [1] | 443 | |
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| 444 | END SUBROUTINE prandtl_fluxes |
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