[97] | 1 | SUBROUTINE diffusivities( var, var_reference ) |
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[1] | 2 | |
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| 3 | !------------------------------------------------------------------------------! |
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[484] | 4 | ! Current revisions: |
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[1] | 5 | ! ----------------- |
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[98] | 6 | ! |
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| 7 | ! |
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| 8 | ! Former revisions: |
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| 9 | ! ----------------- |
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| 10 | ! $Id: diffusivities.f90 510 2010-03-12 00:37:31Z maronga $ |
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| 11 | ! |
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[139] | 12 | ! 137 2007-11-28 08:50:10Z letzel |
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| 13 | ! Bugfix for summation of sums_l_l for flow_statistics |
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| 14 | ! Vertical scalar profiles now based on nzb_s_inner and ngp_2dh_s_inner. |
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| 15 | ! |
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[98] | 16 | ! 97 2007-06-21 08:23:15Z raasch |
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[94] | 17 | ! Adjustment of mixing length calculation for the ocean version. |
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| 18 | ! This is also a bugfix, because the height above the topography is now |
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| 19 | ! used instead of the height above level k=0. |
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[97] | 20 | ! theta renamed var, dpt_dz renamed dvar_dz, +new argument var_reference |
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| 21 | ! use_pt_reference renamed use_reference |
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[77] | 22 | ! |
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| 23 | ! 57 2007-03-09 12:05:41Z raasch |
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| 24 | ! Reference temperature pt_reference can be used in buoyancy term |
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| 25 | ! |
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[3] | 26 | ! RCS Log replace by Id keyword, revision history cleaned up |
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| 27 | ! |
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[1] | 28 | ! Revision 1.24 2006/04/26 12:16:26 raasch |
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| 29 | ! OpenMP optimization (+sums_l_l_t), sqrt_e must be private |
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| 30 | ! |
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| 31 | ! Revision 1.1 1997/09/19 07:41:10 raasch |
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| 32 | ! Initial revision |
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| 33 | ! |
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| 34 | ! |
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| 35 | ! Description: |
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| 36 | ! ------------ |
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| 37 | ! Computation of the turbulent diffusion coefficients for momentum and heat |
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| 38 | ! according to Prandtl-Kolmogorov |
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| 39 | !------------------------------------------------------------------------------! |
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| 40 | |
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| 41 | USE arrays_3d |
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| 42 | USE control_parameters |
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| 43 | USE grid_variables |
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| 44 | USE indices |
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| 45 | USE pegrid |
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| 46 | USE statistics |
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| 47 | |
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| 48 | IMPLICIT NONE |
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| 49 | |
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| 50 | INTEGER :: i, j, k, omp_get_thread_num, sr, tn |
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| 51 | |
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[97] | 52 | REAL :: dvar_dz, l_stable, var_reference |
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[1] | 53 | |
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[97] | 54 | REAL, SAVE :: phi_m = 1.0 |
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[1] | 55 | |
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[97] | 56 | REAL :: var(nzb:nzt+1,nys-1:nyn+1,nxl-1:nxr+1) |
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| 57 | |
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[1] | 58 | REAL, DIMENSION(1:nzt) :: l, ll, sqrt_e |
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| 59 | |
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| 60 | |
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| 61 | ! |
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| 62 | !-- Default thread number in case of one thread |
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| 63 | tn = 0 |
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| 64 | |
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| 65 | ! |
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| 66 | !-- Initialization for calculation of the mixing length profile |
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| 67 | sums_l_l = 0.0 |
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| 68 | |
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| 69 | ! |
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| 70 | !-- Compute the turbulent diffusion coefficient for momentum |
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[97] | 71 | !$OMP PARALLEL PRIVATE (dvar_dz,i,j,k,l,ll,l_stable,phi_m,sqrt_e,sr,tn) |
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[1] | 72 | !$ tn = omp_get_thread_num() |
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| 73 | |
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| 74 | !$OMP DO |
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| 75 | DO i = nxl-1, nxr+1 |
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| 76 | DO j = nys-1, nyn+1 |
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| 77 | |
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| 78 | ! |
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| 79 | !-- Compute the Phi-function for a possible adaption of the mixing length |
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| 80 | !-- to the Prandtl mixing length |
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| 81 | IF ( adjust_mixing_length .AND. prandtl_layer ) THEN |
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| 82 | IF ( rif(j,i) >= 0.0 ) THEN |
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| 83 | phi_m = 1.0 + 5.0 * rif(j,i) |
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| 84 | ELSE |
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| 85 | phi_m = 1.0 / SQRT( SQRT( 1.0 - 16.0 * rif(j,i) ) ) |
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| 86 | ENDIF |
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| 87 | ENDIF |
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| 88 | |
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| 89 | ! |
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| 90 | !-- Introduce an optional minimum tke |
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| 91 | IF ( e_min > 0.0 ) THEN |
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| 92 | DO k = nzb_s_inner(j,i)+1, nzt |
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| 93 | e(k,j,i) = MAX( e(k,j,i), e_min ) |
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| 94 | ENDDO |
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| 95 | ENDIF |
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| 96 | |
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| 97 | ! |
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| 98 | !-- Calculate square root of e in a seperate loop, because it is used |
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| 99 | !-- twice in the next loop (better vectorization) |
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| 100 | DO k = nzb_s_inner(j,i)+1, nzt |
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| 101 | sqrt_e(k) = SQRT( e(k,j,i) ) |
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| 102 | ENDDO |
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| 103 | |
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| 104 | ! |
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| 105 | !-- Determine the mixing length |
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| 106 | DO k = nzb_s_inner(j,i)+1, nzt |
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[97] | 107 | dvar_dz = atmos_ocean_sign * & ! inverse effect of pt/rho gradient |
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| 108 | ( var(k+1,j,i) - var(k-1,j,i) ) * dd2zu(k) |
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| 109 | IF ( dvar_dz > 0.0 ) THEN |
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| 110 | IF ( use_reference ) THEN |
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[57] | 111 | l_stable = 0.76 * sqrt_e(k) / & |
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[97] | 112 | SQRT( g / var_reference * dvar_dz ) + 1E-5 |
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[57] | 113 | ELSE |
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| 114 | l_stable = 0.76 * sqrt_e(k) / & |
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[97] | 115 | SQRT( g / var(k,j,i) * dvar_dz ) + 1E-5 |
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[57] | 116 | ENDIF |
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[1] | 117 | ELSE |
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| 118 | l_stable = l_grid(k) |
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| 119 | ENDIF |
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| 120 | ! |
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| 121 | !-- Adjustment of the mixing length |
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| 122 | IF ( wall_adjustment ) THEN |
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| 123 | l(k) = MIN( l_wall(k,j,i), l_grid(k), l_stable ) |
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| 124 | ll(k) = MIN( l_wall(k,j,i), l_grid(k) ) |
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| 125 | ELSE |
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| 126 | l(k) = MIN( l_grid(k), l_stable ) |
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| 127 | ll(k) = l_grid(k) |
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| 128 | ENDIF |
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| 129 | IF ( adjust_mixing_length .AND. prandtl_layer ) THEN |
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[94] | 130 | l(k) = MIN( l(k), kappa * & |
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| 131 | ( zu(k) - zw(nzb_s_inner(j,i)) ) / phi_m ) |
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| 132 | ll(k) = MIN( ll(k), kappa * & |
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| 133 | ( zu(k) - zw(nzb_s_inner(j,i)) ) / phi_m ) |
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[1] | 134 | ENDIF |
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| 135 | |
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| 136 | ! |
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| 137 | !-- Compute diffusion coefficients for momentum and heat |
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| 138 | km(k,j,i) = 0.1 * l(k) * sqrt_e(k) |
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| 139 | kh(k,j,i) = ( 1.0 + 2.0 * l(k) / ll(k) ) * km(k,j,i) |
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| 140 | |
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| 141 | ENDDO |
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| 142 | |
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| 143 | ! |
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| 144 | !-- Summation for averaged profile (cf. flow_statistics) |
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[137] | 145 | !-- (the IF statement still requires a performance check on NEC machines) |
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[1] | 146 | DO sr = 0, statistic_regions |
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[137] | 147 | IF ( rmask(j,i,sr) /= 0.0 .AND. & |
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| 148 | i >= nxl .AND. i <= nxr .AND. j >= nys .AND. j <= nyn ) THEN |
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[132] | 149 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1] | 150 | sums_l_l(k,sr,tn) = sums_l_l(k,sr,tn) + l(k) |
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| 151 | ENDDO |
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| 152 | ENDIF |
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| 153 | ENDDO |
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| 154 | |
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| 155 | ENDDO |
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| 156 | ENDDO |
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| 157 | |
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| 158 | sums_l_l(nzt+1,:,tn) = sums_l_l(nzt,:,tn) ! quasi boundary-condition for |
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| 159 | ! data output |
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| 160 | |
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| 161 | !$OMP END PARALLEL |
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| 162 | |
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| 163 | ! |
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| 164 | !-- Set vertical boundary values (Neumann conditions both at bottom and top). |
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| 165 | !-- Horizontal boundary conditions at vertical walls are not set because |
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| 166 | !-- so far vertical walls require usage of a Prandtl-layer where the boundary |
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| 167 | !-- values of the diffusivities are not needed |
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| 168 | !$OMP PARALLEL DO |
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| 169 | DO i = nxl-1, nxr+1 |
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| 170 | DO j = nys-1, nyn+1 |
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| 171 | km(nzb_s_inner(j,i),j,i) = km(nzb_s_inner(j,i)+1,j,i) |
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| 172 | km(nzt+1,j,i) = km(nzt,j,i) |
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| 173 | kh(nzb_s_inner(j,i),j,i) = kh(nzb_s_inner(j,i)+1,j,i) |
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| 174 | kh(nzt+1,j,i) = kh(nzt,j,i) |
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| 175 | ENDDO |
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| 176 | ENDDO |
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| 177 | |
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| 178 | ! |
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| 179 | !-- Set Neumann boundary conditions at the outflow boundaries in case of |
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| 180 | !-- non-cyclic lateral boundaries |
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| 181 | IF ( outflow_l ) THEN |
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| 182 | km(:,:,nxl-1) = km(:,:,nxl) |
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| 183 | kh(:,:,nxl-1) = kh(:,:,nxl) |
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| 184 | ENDIF |
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| 185 | IF ( outflow_r ) THEN |
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| 186 | km(:,:,nxr+1) = km(:,:,nxr) |
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| 187 | kh(:,:,nxr+1) = kh(:,:,nxr) |
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| 188 | ENDIF |
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| 189 | IF ( outflow_s ) THEN |
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| 190 | km(:,nys-1,:) = km(:,nys,:) |
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| 191 | kh(:,nys-1,:) = kh(:,nys,:) |
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| 192 | ENDIF |
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| 193 | IF ( outflow_n ) THEN |
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| 194 | km(:,nyn+1,:) = km(:,nyn,:) |
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| 195 | kh(:,nyn+1,:) = kh(:,nyn,:) |
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| 196 | ENDIF |
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| 197 | |
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| 198 | |
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| 199 | END SUBROUTINE diffusivities |
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