| [1] | 1 | MODULE diffusion_v_mod |
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| 2 | |
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| 3 | !------------------------------------------------------------------------------! |
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| 4 | ! Actual revisions: |
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| 5 | ! ----------------- |
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| [102] | 6 | ! Momentumflux at top (vswst) included as boundary condition |
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| [1] | 7 | ! |
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| 8 | ! Former revisions: |
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| 9 | ! ----------------- |
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| [3] | 10 | ! $Id: diffusion_v.f90 103 2007-07-30 10:49:46Z raasch $ |
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| [39] | 11 | ! |
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| [77] | 12 | ! 75 2007-03-22 09:54:05Z raasch |
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| 13 | ! Wall functions now include diabatic conditions, call of routine wall_fluxes, |
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| 14 | ! z0 removed from argument list, vynp eliminated |
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| 15 | ! |
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| [39] | 16 | ! 20 2007-02-26 00:12:32Z raasch |
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| 17 | ! Bugfix: ddzw dimensioned 1:nzt"+1" |
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| 18 | ! |
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| [3] | 19 | ! RCS Log replace by Id keyword, revision history cleaned up |
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| 20 | ! |
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| [1] | 21 | ! Revision 1.15 2006/02/23 10:36:00 raasch |
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| 22 | ! nzb_2d replaced by nzb_v_outer in horizontal diffusion and by nzb_v_inner |
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| 23 | ! or nzb_diff_v, respectively, in vertical diffusion, |
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| 24 | ! wall functions added for north and south walls, +z0 in argument list, |
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| 25 | ! terms containing w(k-1,..) are removed from the Prandtl-layer equation |
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| 26 | ! because they cause errors at the edges of topography |
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| 27 | ! WARNING: loops containing the MAX function are still not properly vectorized! |
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| 28 | ! |
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| 29 | ! Revision 1.1 1997/09/12 06:24:01 raasch |
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| 30 | ! Initial revision |
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| 31 | ! |
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| 32 | ! |
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| 33 | ! Description: |
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| 34 | ! ------------ |
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| 35 | ! Diffusion term of the v-component |
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| 36 | !------------------------------------------------------------------------------! |
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| 37 | |
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| [56] | 38 | USE wall_fluxes_mod |
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| 39 | |
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| [1] | 40 | PRIVATE |
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| 41 | PUBLIC diffusion_v |
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| 42 | |
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| 43 | INTERFACE diffusion_v |
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| 44 | MODULE PROCEDURE diffusion_v |
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| 45 | MODULE PROCEDURE diffusion_v_ij |
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| 46 | END INTERFACE diffusion_v |
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| 47 | |
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| 48 | CONTAINS |
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| 49 | |
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| 50 | |
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| 51 | !------------------------------------------------------------------------------! |
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| 52 | ! Call for all grid points |
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| 53 | !------------------------------------------------------------------------------! |
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| [102] | 54 | SUBROUTINE diffusion_v( ddzu, ddzw, km, km_damp_x, tend, u, v, vsws, & |
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| 55 | vswst, w ) |
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| [1] | 56 | |
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| 57 | USE control_parameters |
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| 58 | USE grid_variables |
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| 59 | USE indices |
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| 60 | |
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| 61 | IMPLICIT NONE |
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| 62 | |
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| 63 | INTEGER :: i, j, k |
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| [51] | 64 | REAL :: kmxm_x, kmxm_y, kmxp_x, kmxp_y, kmzm, kmzp |
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| [20] | 65 | REAL :: ddzu(1:nzt+1), ddzw(1:nzt+1), km_damp_x(nxl-1:nxr+1) |
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| [1] | 66 | REAL :: tend(nzb:nzt+1,nys-1:nyn+1,nxl-1:nxr+1) |
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| [102] | 67 | REAL, DIMENSION(:,:), POINTER :: vsws, vswst |
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| [1] | 68 | REAL, DIMENSION(:,:,:), POINTER :: km, u, v, w |
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| [75] | 69 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: vsus |
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| [1] | 70 | |
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| [56] | 71 | ! |
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| 72 | !-- First calculate horizontal momentum flux v'u' at vertical walls, |
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| 73 | !-- if neccessary |
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| 74 | IF ( topography /= 'flat' ) THEN |
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| [75] | 75 | CALL wall_fluxes( vsus, 0.0, 1.0, 0.0, 0.0, nzb_v_inner, & |
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| [56] | 76 | nzb_v_outer, wall_v ) |
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| 77 | ENDIF |
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| 78 | |
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| [1] | 79 | DO i = nxl, nxr |
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| [75] | 80 | DO j = nys, nyn |
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| [1] | 81 | ! |
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| 82 | !-- Compute horizontal diffusion |
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| 83 | DO k = nzb_v_outer(j,i)+1, nzt |
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| 84 | ! |
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| 85 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 86 | kmxp_x = 0.25 * & |
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| 87 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 88 | kmxm_x = 0.25 * & |
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| 89 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 90 | kmxp_y = kmxp_x |
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| 91 | kmxm_y = kmxm_x |
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| 92 | ! |
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| 93 | !-- Increase diffusion at the outflow boundary in case of |
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| 94 | !-- non-cyclic lateral boundaries. Damping is only needed for |
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| 95 | !-- velocity components parallel to the outflow boundary in |
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| 96 | !-- the direction normal to the outflow boundary. |
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| 97 | IF ( bc_lr /= 'cyclic' ) THEN |
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| 98 | kmxp_x = MAX( kmxp_x, km_damp_x(i) ) |
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| 99 | kmxm_x = MAX( kmxm_x, km_damp_x(i) ) |
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| 100 | ENDIF |
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| 101 | |
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| 102 | tend(k,j,i) = tend(k,j,i) & |
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| 103 | & + ( kmxp_x * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 104 | & + kmxp_y * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 105 | & - kmxm_x * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 106 | & - kmxm_y * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 107 | & ) * ddx & |
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| 108 | & + 2.0 * ( & |
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| 109 | & km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 110 | & - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 111 | & ) * ddy2 |
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| 112 | ENDDO |
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| 113 | |
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| 114 | ! |
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| 115 | !-- Wall functions at the left and right walls, respectively |
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| 116 | IF ( wall_v(j,i) /= 0.0 ) THEN |
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| [51] | 117 | |
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| [1] | 118 | DO k = nzb_v_inner(j,i)+1, nzb_v_outer(j,i) |
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| 119 | kmxp_x = 0.25 * & |
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| 120 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 121 | kmxm_x = 0.25 * & |
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| 122 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 123 | kmxp_y = kmxp_x |
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| 124 | kmxm_y = kmxm_x |
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| 125 | ! |
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| 126 | !-- Increase diffusion at the outflow boundary in case of |
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| 127 | !-- non-cyclic lateral boundaries. Damping is only needed for |
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| 128 | !-- velocity components parallel to the outflow boundary in |
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| 129 | !-- the direction normal to the outflow boundary. |
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| 130 | IF ( bc_lr /= 'cyclic' ) THEN |
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| 131 | kmxp_x = MAX( kmxp_x, km_damp_x(i) ) |
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| 132 | kmxm_x = MAX( kmxm_x, km_damp_x(i) ) |
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| 133 | ENDIF |
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| 134 | |
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| 135 | tend(k,j,i) = tend(k,j,i) & |
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| 136 | + 2.0 * ( & |
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| 137 | km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 138 | - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 139 | ) * ddy2 & |
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| 140 | + ( fxp(j,i) * ( & |
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| 141 | kmxp_x * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 142 | + kmxp_y * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 143 | ) & |
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| 144 | - fxm(j,i) * ( & |
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| 145 | kmxm_x * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 146 | + kmxm_y * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 147 | ) & |
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| [56] | 148 | + wall_v(j,i) * vsus(k,j,i) & |
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| [1] | 149 | ) * ddx |
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| 150 | ENDDO |
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| 151 | ENDIF |
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| 152 | |
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| 153 | ! |
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| 154 | !-- Compute vertical diffusion. In case of simulating a Prandtl |
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| 155 | !-- layer, index k starts at nzb_v_inner+2. |
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| [102] | 156 | DO k = nzb_diff_v(j,i), nzt_diff |
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| [1] | 157 | ! |
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| 158 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 159 | kmzp = 0.25 * & |
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| 160 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 161 | kmzm = 0.25 * & |
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| 162 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 163 | |
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| 164 | tend(k,j,i) = tend(k,j,i) & |
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| 165 | & + ( kmzp * ( ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| 166 | & + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 167 | & ) & |
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| 168 | & - kmzm * ( ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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| 169 | & + ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 170 | & ) & |
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| 171 | & ) * ddzw(k) |
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| 172 | ENDDO |
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| 173 | |
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| 174 | ! |
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| 175 | !-- Vertical diffusion at the first grid point above the surface, |
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| 176 | !-- if the momentum flux at the bottom is given by the Prandtl law |
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| 177 | !-- or if it is prescribed by the user. |
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| 178 | !-- Difference quotient of the momentum flux is not formed over |
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| 179 | !-- half of the grid spacing (2.0*ddzw(k)) any more, since the |
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| 180 | !-- comparison with other (LES) modell showed that the values of |
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| 181 | !-- the momentum flux becomes too large in this case. |
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| 182 | !-- The term containing w(k-1,..) (see above equation) is removed here |
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| 183 | !-- because the vertical velocity is assumed to be zero at the surface. |
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| 184 | IF ( use_surface_fluxes ) THEN |
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| 185 | k = nzb_v_inner(j,i)+1 |
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| 186 | ! |
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| 187 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 188 | kmzp = 0.25 * & |
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| 189 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 190 | kmzm = 0.25 * & |
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| 191 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 192 | |
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| 193 | tend(k,j,i) = tend(k,j,i) & |
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| 194 | & + ( kmzp * ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 195 | & ) * ddzw(k) & |
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| [102] | 196 | & + ( kmzp * ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| [1] | 197 | & + vsws(j,i) & |
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| 198 | & ) * ddzw(k) |
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| 199 | ENDIF |
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| 200 | |
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| [102] | 201 | ! |
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| 202 | !-- Vertical diffusion at the first gridpoint below the top boundary, |
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| 203 | !-- if the momentum flux at the top is prescribed by the user |
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| [103] | 204 | IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN |
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| [102] | 205 | k = nzt |
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| 206 | ! |
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| 207 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 208 | kmzp = 0.25 * & |
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| 209 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 210 | kmzm = 0.25 * & |
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| 211 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 212 | |
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| 213 | tend(k,j,i) = tend(k,j,i) & |
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| 214 | & - ( kmzm * ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 215 | & ) * ddzw(k) & |
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| 216 | & + ( -vswst(j,i) & |
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| 217 | & - kmzm * ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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| 218 | & ) * ddzw(k) |
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| 219 | ENDIF |
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| 220 | |
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| [1] | 221 | ENDDO |
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| 222 | ENDDO |
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| 223 | |
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| 224 | END SUBROUTINE diffusion_v |
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| 225 | |
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| 226 | |
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| 227 | !------------------------------------------------------------------------------! |
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| 228 | ! Call for grid point i,j |
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| 229 | !------------------------------------------------------------------------------! |
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| 230 | SUBROUTINE diffusion_v_ij( i, j, ddzu, ddzw, km, km_damp_x, tend, u, v, & |
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| [102] | 231 | vsws, vswst, w ) |
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| [1] | 232 | |
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| 233 | USE control_parameters |
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| 234 | USE grid_variables |
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| 235 | USE indices |
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| 236 | |
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| 237 | IMPLICIT NONE |
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| 238 | |
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| 239 | INTEGER :: i, j, k |
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| [51] | 240 | REAL :: kmxm_x, kmxm_y, kmxp_x, kmxp_y, kmzm, kmzp |
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| [20] | 241 | REAL :: ddzu(1:nzt+1), ddzw(1:nzt+1), km_damp_x(nxl-1:nxr+1) |
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| [1] | 242 | REAL :: tend(nzb:nzt+1,nys-1:nyn+1,nxl-1:nxr+1) |
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| [51] | 243 | REAL, DIMENSION(nzb:nzt+1) :: vsus |
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| [102] | 244 | REAL, DIMENSION(:,:), POINTER :: vsws, vswst |
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| [1] | 245 | REAL, DIMENSION(:,:,:), POINTER :: km, u, v, w |
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| 246 | |
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| 247 | ! |
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| 248 | !-- Compute horizontal diffusion |
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| 249 | DO k = nzb_v_outer(j,i)+1, nzt |
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| 250 | ! |
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| 251 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 252 | kmxp_x = 0.25 * ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 253 | kmxm_x = 0.25 * ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 254 | kmxp_y = kmxp_x |
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| 255 | kmxm_y = kmxm_x |
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| 256 | ! |
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| 257 | !-- Increase diffusion at the outflow boundary in case of non-cyclic |
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| 258 | !-- lateral boundaries. Damping is only needed for velocity components |
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| 259 | !-- parallel to the outflow boundary in the direction normal to the |
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| 260 | !-- outflow boundary. |
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| 261 | IF ( bc_lr /= 'cyclic' ) THEN |
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| 262 | kmxp_x = MAX( kmxp_x, km_damp_x(i) ) |
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| 263 | kmxm_x = MAX( kmxm_x, km_damp_x(i) ) |
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| 264 | ENDIF |
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| 265 | |
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| 266 | tend(k,j,i) = tend(k,j,i) & |
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| 267 | & + ( kmxp_x * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 268 | & + kmxp_y * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 269 | & - kmxm_x * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 270 | & - kmxm_y * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 271 | & ) * ddx & |
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| 272 | & + 2.0 * ( & |
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| 273 | & km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 274 | & - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 275 | & ) * ddy2 |
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| 276 | ENDDO |
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| 277 | |
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| 278 | ! |
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| 279 | !-- Wall functions at the left and right walls, respectively |
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| 280 | IF ( wall_v(j,i) /= 0.0 ) THEN |
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| [51] | 281 | |
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| 282 | ! |
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| 283 | !-- Calculate the horizontal momentum flux v'u' |
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| 284 | CALL wall_fluxes( i, j, nzb_v_inner(j,i)+1, nzb_v_outer(j,i), & |
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| 285 | vsus, 0.0, 1.0, 0.0, 0.0 ) |
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| 286 | |
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| [1] | 287 | DO k = nzb_v_inner(j,i)+1, nzb_v_outer(j,i) |
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| 288 | kmxp_x = 0.25 * & |
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| 289 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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| 290 | kmxm_x = 0.25 * & |
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| 291 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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| 292 | kmxp_y = kmxp_x |
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| 293 | kmxm_y = kmxm_x |
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| 294 | ! |
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| 295 | !-- Increase diffusion at the outflow boundary in case of |
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| 296 | !-- non-cyclic lateral boundaries. Damping is only needed for |
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| 297 | !-- velocity components parallel to the outflow boundary in |
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| 298 | !-- the direction normal to the outflow boundary. |
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| 299 | IF ( bc_lr /= 'cyclic' ) THEN |
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| 300 | kmxp_x = MAX( kmxp_x, km_damp_x(i) ) |
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| 301 | kmxm_x = MAX( kmxm_x, km_damp_x(i) ) |
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| 302 | ENDIF |
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| 303 | |
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| 304 | tend(k,j,i) = tend(k,j,i) & |
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| 305 | + 2.0 * ( & |
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| 306 | km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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| 307 | - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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| 308 | ) * ddy2 & |
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| 309 | + ( fxp(j,i) * ( & |
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| 310 | kmxp_x * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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| 311 | + kmxp_y * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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| 312 | ) & |
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| 313 | - fxm(j,i) * ( & |
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| 314 | kmxm_x * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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| 315 | + kmxm_y * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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| 316 | ) & |
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| [51] | 317 | + wall_v(j,i) * vsus(k) & |
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| [1] | 318 | ) * ddx |
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| 319 | ENDDO |
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| 320 | ENDIF |
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| 321 | |
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| 322 | ! |
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| 323 | !-- Compute vertical diffusion. In case of simulating a Prandtl layer, |
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| 324 | !-- index k starts at nzb_v_inner+2. |
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| [102] | 325 | DO k = nzb_diff_v(j,i), nzt_diff |
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| [1] | 326 | ! |
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| 327 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 328 | kmzp = 0.25 * ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 329 | kmzm = 0.25 * ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 330 | |
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| 331 | tend(k,j,i) = tend(k,j,i) & |
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| 332 | & + ( kmzp * ( ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| 333 | & + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 334 | & ) & |
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| 335 | & - kmzm * ( ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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| 336 | & + ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 337 | & ) & |
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| 338 | & ) * ddzw(k) |
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| 339 | ENDDO |
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| 340 | |
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| 341 | ! |
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| 342 | !-- Vertical diffusion at the first grid point above the surface, if the |
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| 343 | !-- momentum flux at the bottom is given by the Prandtl law or if it is |
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| 344 | !-- prescribed by the user. |
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| 345 | !-- Difference quotient of the momentum flux is not formed over half of |
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| 346 | !-- the grid spacing (2.0*ddzw(k)) any more, since the comparison with |
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| 347 | !-- other (LES) modell showed that the values of the momentum flux becomes |
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| 348 | !-- too large in this case. |
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| 349 | !-- The term containing w(k-1,..) (see above equation) is removed here |
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| 350 | !-- because the vertical velocity is assumed to be zero at the surface. |
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| 351 | IF ( use_surface_fluxes ) THEN |
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| 352 | k = nzb_v_inner(j,i)+1 |
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| 353 | ! |
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| 354 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 355 | kmzp = 0.25 * ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 356 | kmzm = 0.25 * ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 357 | |
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| 358 | tend(k,j,i) = tend(k,j,i) & |
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| 359 | & + ( kmzp * ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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| 360 | & ) * ddzw(k) & |
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| [102] | 361 | & + ( kmzp * ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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| [1] | 362 | & + vsws(j,i) & |
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| 363 | & ) * ddzw(k) |
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| 364 | ENDIF |
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| 365 | |
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| [102] | 366 | ! |
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| 367 | !-- Vertical diffusion at the first gridpoint below the top boundary, |
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| 368 | !-- if the momentum flux at the top is prescribed by the user |
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| [103] | 369 | IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN |
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| [102] | 370 | k = nzt |
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| 371 | ! |
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| 372 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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| 373 | kmzp = 0.25 * & |
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| 374 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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| 375 | kmzm = 0.25 * & |
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| 376 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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| 377 | |
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| 378 | tend(k,j,i) = tend(k,j,i) & |
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| 379 | & - ( kmzm * ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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| 380 | & ) * ddzw(k) & |
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| 381 | & + ( -vswst(j,i) & |
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| 382 | & - kmzm * ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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| 383 | & ) * ddzw(k) |
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| 384 | ENDIF |
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| 385 | |
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| [1] | 386 | END SUBROUTINE diffusion_v_ij |
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| 387 | |
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| 388 | END MODULE diffusion_v_mod |
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