[56] | 1 | MODULE wall_fluxes_mod |
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[52] | 2 | !------------------------------------------------------------------------------! |
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[484] | 3 | ! Current revisions: |
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[52] | 4 | ! ----------------- |
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[198] | 5 | ! |
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| 6 | ! |
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| 7 | ! Former revisions: |
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| 8 | ! ----------------- |
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| 9 | ! $Id: wall_fluxes.f90 484 2010-02-05 07:36:54Z heinze $ |
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| 10 | ! |
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| 11 | ! 187 2008-08-06 16:25:09Z letzel |
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| 12 | ! Bugfix: Modification of the evaluation of the vertical turbulent momentum |
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| 13 | ! fluxes u'w' and v'w (see prandtl_fluxes), this requires the calculation of |
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| 14 | ! us_wall (and vel_total, u_i, v_i, ws) also in wall_fluxes_e. |
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| 15 | ! Bugfix: change definition of us_wall from 1D to 2D |
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[187] | 16 | ! Bugfix: storage of rifs to rifs_wall in wall_fluxes_e removed |
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| 17 | ! Change: add 'minus' sign to fluxes produced by subroutine wall_fluxes_e for |
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[198] | 18 | ! consistency with subroutine wall_fluxes |
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[187] | 19 | ! Change: Modification of the integrated version of the profile function for |
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[198] | 20 | ! momentum for unstable stratification |
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[52] | 21 | ! |
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| 22 | ! Initial version (2007/03/07) |
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| 23 | ! |
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| 24 | ! Description: |
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| 25 | ! ------------ |
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| 26 | ! Calculates momentum fluxes at vertical walls assuming Monin-Obukhov |
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| 27 | ! similarity. |
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| 28 | ! Indices: usvs a=1, vsus b=1, wsvs c1=1, wsus c2=1 (other=0). |
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[56] | 29 | ! The all-gridpoint version of wall_fluxes_e is not used so far, because |
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| 30 | ! it gives slightly different results from the ij-version for some unknown |
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| 31 | ! reason. |
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[52] | 32 | !------------------------------------------------------------------------------! |
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[56] | 33 | PRIVATE |
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| 34 | PUBLIC wall_fluxes, wall_fluxes_e |
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| 35 | |
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| 36 | INTERFACE wall_fluxes |
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| 37 | MODULE PROCEDURE wall_fluxes |
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| 38 | MODULE PROCEDURE wall_fluxes_ij |
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| 39 | END INTERFACE wall_fluxes |
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| 40 | |
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| 41 | INTERFACE wall_fluxes_e |
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| 42 | MODULE PROCEDURE wall_fluxes_e |
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| 43 | MODULE PROCEDURE wall_fluxes_e_ij |
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| 44 | END INTERFACE wall_fluxes_e |
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| 45 | |
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| 46 | CONTAINS |
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[52] | 47 | |
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[56] | 48 | !------------------------------------------------------------------------------! |
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| 49 | ! Call for all grid points |
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| 50 | !------------------------------------------------------------------------------! |
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[75] | 51 | SUBROUTINE wall_fluxes( wall_flux, a, b, c1, c2, nzb_uvw_inner, & |
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[56] | 52 | nzb_uvw_outer, wall ) |
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[52] | 53 | |
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[56] | 54 | USE arrays_3d |
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| 55 | USE control_parameters |
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| 56 | USE grid_variables |
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| 57 | USE indices |
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| 58 | USE statistics |
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[52] | 59 | |
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[56] | 60 | IMPLICIT NONE |
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[52] | 61 | |
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[75] | 62 | INTEGER :: i, j, k, wall_index |
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[52] | 63 | |
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[56] | 64 | INTEGER, DIMENSION(nys-1:nyn+1,nxl-1:nxr+1) :: nzb_uvw_inner, & |
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| 65 | nzb_uvw_outer |
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| 66 | REAL :: a, b, c1, c2, h1, h2, zp |
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| 67 | REAL :: pts, pt_i, rifs, u_i, v_i, us_wall, vel_total, ws, wspts |
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[52] | 68 | |
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[75] | 69 | REAL, DIMENSION(nys-1:nyn+1,nxl-1:nxr+1) :: wall |
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| 70 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
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[52] | 71 | |
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| 72 | |
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[56] | 73 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 74 | wall_flux = 0.0 |
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| 75 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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| 76 | |
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[75] | 77 | DO i = nxl, nxr |
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| 78 | DO j = nys, nyn |
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[56] | 79 | |
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| 80 | IF ( wall(j,i) /= 0.0 ) THEN |
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[52] | 81 | ! |
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[56] | 82 | !-- All subsequent variables are computed for the respective |
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[187] | 83 | !-- location where the respective flux is defined. |
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[56] | 84 | DO k = nzb_uvw_inner(j,i)+1, nzb_uvw_outer(j,i) |
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[53] | 85 | |
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[52] | 86 | ! |
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[56] | 87 | !-- (1) Compute rifs, u_i, v_i, ws, pt' and w'pt' |
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| 88 | rifs = rif_wall(k,j,i,wall_index) |
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[53] | 89 | |
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[56] | 90 | u_i = a * u(k,j,i) + c1 * 0.25 * & |
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| 91 | ( u(k+1,j,i+1) + u(k+1,j,i) + u(k,j,i+1) + u(k,j,i) ) |
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[53] | 92 | |
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[56] | 93 | v_i = b * v(k,j,i) + c2 * 0.25 * & |
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| 94 | ( v(k+1,j+1,i) + v(k+1,j,i) + v(k,j+1,i) + v(k,j,i) ) |
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[53] | 95 | |
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[56] | 96 | ws = ( c1 + c2 ) * w(k,j,i) + 0.25 * ( & |
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| 97 | a * ( w(k-1,j,i-1) + w(k-1,j,i) + w(k,j,i-1) + w(k,j,i) ) & |
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| 98 | + b * ( w(k-1,j-1,i) + w(k-1,j,i) + w(k,j-1,i) + w(k,j,i) ) & |
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| 99 | ) |
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| 100 | pt_i = 0.5 * ( pt(k,j,i) + a * pt(k,j,i-1) + & |
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| 101 | b * pt(k,j-1,i) + ( c1 + c2 ) * pt(k+1,j,i) ) |
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[53] | 102 | |
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[56] | 103 | pts = pt_i - hom(k,1,4,0) |
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| 104 | wspts = ws * pts |
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[53] | 105 | |
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[52] | 106 | ! |
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[56] | 107 | !-- (2) Compute wall-parallel absolute velocity vel_total |
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| 108 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
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[53] | 109 | |
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[52] | 110 | ! |
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[56] | 111 | !-- (3) Compute wall friction velocity us_wall |
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| 112 | IF ( rifs >= 0.0 ) THEN |
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[53] | 113 | |
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[52] | 114 | ! |
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[56] | 115 | !-- Stable stratification (and neutral) |
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| 116 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 117 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 118 | ) |
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| 119 | ELSE |
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[53] | 120 | |
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[52] | 121 | ! |
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[56] | 122 | !-- Unstable stratification |
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[187] | 123 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 124 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[53] | 125 | |
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[187] | 126 | us_wall = kappa * vel_total / ( & |
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| 127 | LOG( zp / z0(j,i) ) - & |
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| 128 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 129 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 130 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 131 | ) |
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[56] | 132 | ENDIF |
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[53] | 133 | |
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[52] | 134 | ! |
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[56] | 135 | !-- (4) Compute zp/L (corresponds to neutral Richardson flux |
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| 136 | !-- number rifs) |
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| 137 | rifs = -1.0 * zp * kappa * g * wspts / ( pt_i * & |
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| 138 | ( us_wall**3 + 1E-30 ) ) |
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[53] | 139 | |
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[52] | 140 | ! |
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[56] | 141 | !-- Limit the value range of the Richardson numbers. |
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| 142 | !-- This is necessary for very small velocities (u,w --> 0), |
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| 143 | !-- because the absolute value of rif can then become very |
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| 144 | !-- large, which in consequence would result in very large |
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| 145 | !-- shear stresses and very small momentum fluxes (both are |
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| 146 | !-- generally unrealistic). |
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| 147 | IF ( rifs < rif_min ) rifs = rif_min |
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| 148 | IF ( rifs > rif_max ) rifs = rif_max |
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[53] | 149 | |
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[52] | 150 | ! |
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[56] | 151 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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| 152 | IF ( rifs >= 0.0 ) THEN |
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[53] | 153 | |
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[52] | 154 | ! |
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[56] | 155 | !-- Stable stratification (and neutral) |
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| 156 | wall_flux(k,j,i) = kappa * & |
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| 157 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / & |
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| 158 | ( LOG( zp / z0(j,i) ) + & |
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| 159 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 160 | ) |
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| 161 | ELSE |
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[53] | 162 | |
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[52] | 163 | ! |
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[56] | 164 | !-- Unstable stratification |
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[187] | 165 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 166 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[53] | 167 | |
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[187] | 168 | wall_flux(k,j,i) = kappa * & |
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| 169 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / ( & |
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| 170 | LOG( zp / z0(j,i) ) - & |
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| 171 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 172 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 173 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 174 | ) |
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[56] | 175 | ENDIF |
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[187] | 176 | wall_flux(k,j,i) = -wall_flux(k,j,i) * us_wall |
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[56] | 177 | |
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| 178 | ! |
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| 179 | !-- store rifs for next time step |
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| 180 | rif_wall(k,j,i,wall_index) = rifs |
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| 181 | |
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| 182 | ENDDO |
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| 183 | |
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| 184 | ENDIF |
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| 185 | |
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| 186 | ENDDO |
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| 187 | ENDDO |
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| 188 | |
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| 189 | END SUBROUTINE wall_fluxes |
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| 190 | |
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| 191 | |
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| 192 | |
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| 193 | !------------------------------------------------------------------------------! |
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| 194 | ! Call for all grid point i,j |
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| 195 | !------------------------------------------------------------------------------! |
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| 196 | SUBROUTINE wall_fluxes_ij( i, j, nzb_w, nzt_w, wall_flux, a, b, c1, c2 ) |
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| 197 | |
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| 198 | USE arrays_3d |
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| 199 | USE control_parameters |
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| 200 | USE grid_variables |
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| 201 | USE indices |
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| 202 | USE statistics |
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| 203 | |
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| 204 | IMPLICIT NONE |
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| 205 | |
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| 206 | INTEGER :: i, j, k, nzb_w, nzt_w, wall_index |
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| 207 | REAL :: a, b, c1, c2, h1, h2, zp |
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| 208 | |
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| 209 | REAL :: pts, pt_i, rifs, u_i, v_i, us_wall, vel_total, ws, wspts |
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| 210 | |
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| 211 | REAL, DIMENSION(nzb:nzt+1) :: wall_flux |
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| 212 | |
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| 213 | |
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| 214 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 215 | wall_flux = 0.0 |
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| 216 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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| 217 | |
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| 218 | ! |
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| 219 | !-- All subsequent variables are computed for the respective location where |
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[187] | 220 | !-- the respective flux is defined. |
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[56] | 221 | DO k = nzb_w, nzt_w |
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| 222 | |
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| 223 | ! |
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| 224 | !-- (1) Compute rifs, u_i, v_i, ws, pt' and w'pt' |
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| 225 | rifs = rif_wall(k,j,i,wall_index) |
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| 226 | |
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| 227 | u_i = a * u(k,j,i) + c1 * 0.25 * & |
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| 228 | ( u(k+1,j,i+1) + u(k+1,j,i) + u(k,j,i+1) + u(k,j,i) ) |
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| 229 | |
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| 230 | v_i = b * v(k,j,i) + c2 * 0.25 * & |
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| 231 | ( v(k+1,j+1,i) + v(k+1,j,i) + v(k,j+1,i) + v(k,j,i) ) |
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| 232 | |
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| 233 | ws = ( c1 + c2 ) * w(k,j,i) + 0.25 * ( & |
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| 234 | a * ( w(k-1,j,i-1) + w(k-1,j,i) + w(k,j,i-1) + w(k,j,i) ) & |
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| 235 | + b * ( w(k-1,j-1,i) + w(k-1,j,i) + w(k,j-1,i) + w(k,j,i) ) & |
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| 236 | ) |
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| 237 | pt_i = 0.5 * ( pt(k,j,i) + a * pt(k,j,i-1) + b * pt(k,j-1,i) & |
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| 238 | + ( c1 + c2 ) * pt(k+1,j,i) ) |
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| 239 | |
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| 240 | pts = pt_i - hom(k,1,4,0) |
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| 241 | wspts = ws * pts |
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| 242 | |
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| 243 | ! |
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| 244 | !-- (2) Compute wall-parallel absolute velocity vel_total |
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| 245 | vel_total = SQRT( ws**2 + ( a+c1 ) * u_i**2 + ( b+c2 ) * v_i**2 ) |
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| 246 | |
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| 247 | ! |
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| 248 | !-- (3) Compute wall friction velocity us_wall |
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| 249 | IF ( rifs >= 0.0 ) THEN |
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| 250 | |
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| 251 | ! |
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| 252 | !-- Stable stratification (and neutral) |
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| 253 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 254 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 255 | ) |
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| 256 | ELSE |
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| 257 | |
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| 258 | ! |
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| 259 | !-- Unstable stratification |
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[187] | 260 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 261 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[56] | 262 | |
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[187] | 263 | us_wall = kappa * vel_total / ( & |
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| 264 | LOG( zp / z0(j,i) ) - & |
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| 265 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 266 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 267 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 268 | ) |
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[56] | 269 | ENDIF |
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| 270 | |
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| 271 | ! |
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| 272 | !-- (4) Compute zp/L (corresponds to neutral Richardson flux number |
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| 273 | !-- rifs) |
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| 274 | rifs = -1.0 * zp * kappa * g * wspts / ( pt_i * (us_wall**3 + 1E-30) ) |
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| 275 | |
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| 276 | ! |
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| 277 | !-- Limit the value range of the Richardson numbers. |
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| 278 | !-- This is necessary for very small velocities (u,w --> 0), because |
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| 279 | !-- the absolute value of rif can then become very large, which in |
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| 280 | !-- consequence would result in very large shear stresses and very |
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| 281 | !-- small momentum fluxes (both are generally unrealistic). |
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| 282 | IF ( rifs < rif_min ) rifs = rif_min |
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| 283 | IF ( rifs > rif_max ) rifs = rif_max |
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| 284 | |
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| 285 | ! |
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| 286 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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| 287 | IF ( rifs >= 0.0 ) THEN |
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| 288 | |
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| 289 | ! |
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| 290 | !-- Stable stratification (and neutral) |
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[53] | 291 | wall_flux(k) = kappa * & |
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| 292 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / & |
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[56] | 293 | ( LOG( zp / z0(j,i) ) + & |
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| 294 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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[53] | 295 | ) |
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[52] | 296 | ELSE |
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[53] | 297 | |
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[56] | 298 | ! |
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| 299 | !-- Unstable stratification |
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[187] | 300 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 301 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[52] | 302 | |
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[187] | 303 | wall_flux(k) = kappa * & |
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| 304 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / ( & |
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| 305 | LOG( zp / z0(j,i) ) - & |
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| 306 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 307 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 308 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 309 | ) |
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[56] | 310 | ENDIF |
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[187] | 311 | wall_flux(k) = -wall_flux(k) * us_wall |
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[53] | 312 | |
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[56] | 313 | ! |
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| 314 | !-- store rifs for next time step |
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| 315 | rif_wall(k,j,i,wall_index) = rifs |
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[53] | 316 | |
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[56] | 317 | ENDDO |
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[53] | 318 | |
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[56] | 319 | END SUBROUTINE wall_fluxes_ij |
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[53] | 320 | |
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[56] | 321 | |
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| 322 | |
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[53] | 323 | !------------------------------------------------------------------------------! |
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[56] | 324 | ! Call for all grid points |
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| 325 | !------------------------------------------------------------------------------! |
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| 326 | SUBROUTINE wall_fluxes_e( wall_flux, a, b, c1, c2, wall ) |
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| 327 | |
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| 328 | !------------------------------------------------------------------------------! |
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[53] | 329 | ! Description: |
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| 330 | ! ------------ |
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| 331 | ! Calculates momentum fluxes at vertical walls for routine production_e |
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| 332 | ! assuming Monin-Obukhov similarity. |
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| 333 | ! Indices: usvs a=1, vsus b=1, wsvs c1=1, wsus c2=1 (other=0). |
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| 334 | !------------------------------------------------------------------------------! |
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| 335 | |
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[56] | 336 | USE arrays_3d |
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| 337 | USE control_parameters |
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| 338 | USE grid_variables |
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| 339 | USE indices |
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| 340 | USE statistics |
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[53] | 341 | |
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[56] | 342 | IMPLICIT NONE |
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[53] | 343 | |
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[56] | 344 | INTEGER :: i, j, k, kk, wall_index |
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[187] | 345 | REAL :: a, b, c1, c2, h1, h2, u_i, v_i, us_wall, vel_total, vel_zp, & |
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| 346 | ws, zp |
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[53] | 347 | |
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[56] | 348 | REAL :: rifs |
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[53] | 349 | |
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[56] | 350 | REAL, DIMENSION(nys-1:nyn+1,nxl-1:nxr+1) :: wall |
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| 351 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
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[53] | 352 | |
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| 353 | |
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[56] | 354 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 355 | wall_flux = 0.0 |
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| 356 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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[53] | 357 | |
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[56] | 358 | DO i = nxl, nxr |
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| 359 | DO j = nys, nyn |
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| 360 | |
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| 361 | IF ( wall(j,i) /= 0.0 ) THEN |
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[53] | 362 | ! |
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[187] | 363 | !-- All subsequent variables are computed for scalar locations. |
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[56] | 364 | DO k = nzb_diff_s_inner(j,i)-1, nzb_diff_s_outer(j,i)-2 |
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[53] | 365 | ! |
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[187] | 366 | !-- (1) Compute rifs, u_i, v_i, and ws |
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[56] | 367 | IF ( k == nzb_diff_s_inner(j,i)-1 ) THEN |
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| 368 | kk = nzb_diff_s_inner(j,i)-1 |
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| 369 | ELSE |
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| 370 | kk = k-1 |
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| 371 | ENDIF |
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| 372 | rifs = 0.5 * ( rif_wall(k,j,i,wall_index) + & |
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| 373 | a * rif_wall(k,j,i+1,1) + b * rif_wall(k,j+1,i,2) + & |
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| 374 | c1 * rif_wall(kk,j,i,3) + c2 * rif_wall(kk,j,i,4) & |
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| 375 | ) |
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[53] | 376 | |
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[187] | 377 | u_i = 0.5 * ( u(k,j,i) + u(k,j,i+1) ) |
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| 378 | v_i = 0.5 * ( v(k,j,i) + v(k,j+1,i) ) |
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| 379 | ws = 0.5 * ( w(k,j,i) + w(k-1,j,i) ) |
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[53] | 380 | ! |
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[187] | 381 | !-- (2) Compute wall-parallel absolute velocity vel_total and |
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| 382 | !-- interpolate appropriate velocity component vel_zp. |
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| 383 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
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| 384 | vel_zp = 0.5 * ( a * u_i + b * v_i + (c1+c2) * ws ) |
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| 385 | ! |
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| 386 | !-- (3) Compute wall friction velocity us_wall |
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| 387 | IF ( rifs >= 0.0 ) THEN |
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[53] | 388 | |
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| 389 | ! |
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[187] | 390 | !-- Stable stratification (and neutral) |
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| 391 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 392 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 393 | ) |
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| 394 | ELSE |
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| 395 | |
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| 396 | ! |
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| 397 | !-- Unstable stratification |
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| 398 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 399 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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| 400 | |
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| 401 | us_wall = kappa * vel_total / ( & |
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| 402 | LOG( zp / z0(j,i) ) - & |
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| 403 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 404 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 405 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 406 | ) |
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| 407 | ENDIF |
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| 408 | |
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| 409 | ! |
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| 410 | !-- Skip step (4) of wall_fluxes, because here rifs is already |
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| 411 | !-- available from (1) |
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| 412 | ! |
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[56] | 413 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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[55] | 414 | |
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[56] | 415 | IF ( rifs >= 0.0 ) THEN |
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[53] | 416 | |
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| 417 | ! |
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[56] | 418 | !-- Stable stratification (and neutral) |
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| 419 | wall_flux(k,j,i) = kappa * vel_zp / & |
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| 420 | ( LOG( zp/z0(j,i) ) + 5.0*rifs * ( zp-z0(j,i) ) / zp ) |
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| 421 | ELSE |
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[53] | 422 | |
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| 423 | ! |
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[56] | 424 | !-- Unstable stratification |
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[187] | 425 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 426 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[53] | 427 | |
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[187] | 428 | wall_flux(k,j,i) = kappa * vel_zp / ( & |
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| 429 | LOG( zp / z0(j,i) ) - & |
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| 430 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 431 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 432 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 433 | ) |
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[56] | 434 | ENDIF |
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[187] | 435 | wall_flux(k,j,i) = - wall_flux(k,j,i) * us_wall |
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[56] | 436 | |
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| 437 | ENDDO |
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| 438 | |
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| 439 | ENDIF |
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| 440 | |
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| 441 | ENDDO |
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| 442 | ENDDO |
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| 443 | |
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| 444 | END SUBROUTINE wall_fluxes_e |
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| 445 | |
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| 446 | |
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| 447 | |
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| 448 | !------------------------------------------------------------------------------! |
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| 449 | ! Call for grid point i,j |
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| 450 | !------------------------------------------------------------------------------! |
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| 451 | SUBROUTINE wall_fluxes_e_ij( i, j, nzb_w, nzt_w, wall_flux, a, b, c1, c2 ) |
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| 452 | |
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| 453 | USE arrays_3d |
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| 454 | USE control_parameters |
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| 455 | USE grid_variables |
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| 456 | USE indices |
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| 457 | USE statistics |
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| 458 | |
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| 459 | IMPLICIT NONE |
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| 460 | |
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| 461 | INTEGER :: i, j, k, kk, nzb_w, nzt_w, wall_index |
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[187] | 462 | REAL :: a, b, c1, c2, h1, h2, u_i, v_i, us_wall, vel_total, vel_zp, & |
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| 463 | ws, zp |
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[56] | 464 | |
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| 465 | REAL :: rifs |
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| 466 | |
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| 467 | REAL, DIMENSION(nzb:nzt+1) :: wall_flux |
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| 468 | |
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| 469 | |
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| 470 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
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| 471 | wall_flux = 0.0 |
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| 472 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
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| 473 | |
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| 474 | ! |
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[187] | 475 | !-- All subsequent variables are computed for scalar locations. |
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[56] | 476 | DO k = nzb_w, nzt_w |
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| 477 | |
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| 478 | ! |
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[187] | 479 | !-- (1) Compute rifs, u_i, v_i, and ws |
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[56] | 480 | IF ( k == nzb_w ) THEN |
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| 481 | kk = nzb_w |
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[53] | 482 | ELSE |
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[56] | 483 | kk = k-1 |
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| 484 | ENDIF |
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| 485 | rifs = 0.5 * ( rif_wall(k,j,i,wall_index) + & |
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| 486 | a * rif_wall(k,j,i+1,1) + b * rif_wall(k,j+1,i,2) + & |
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| 487 | c1 * rif_wall(kk,j,i,3) + c2 * rif_wall(kk,j,i,4) & |
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| 488 | ) |
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| 489 | |
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[187] | 490 | u_i = 0.5 * ( u(k,j,i) + u(k,j,i+1) ) |
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| 491 | v_i = 0.5 * ( v(k,j,i) + v(k,j+1,i) ) |
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| 492 | ws = 0.5 * ( w(k,j,i) + w(k-1,j,i) ) |
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[56] | 493 | ! |
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[187] | 494 | !-- (2) Compute wall-parallel absolute velocity vel_total and |
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| 495 | !-- interpolate appropriate velocity component vel_zp. |
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| 496 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
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| 497 | vel_zp = 0.5 * ( a * u_i + b * v_i + (c1+c2) * ws ) |
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| 498 | ! |
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| 499 | !-- (3) Compute wall friction velocity us_wall |
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| 500 | IF ( rifs >= 0.0 ) THEN |
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[56] | 501 | |
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| 502 | ! |
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[187] | 503 | !-- Stable stratification (and neutral) |
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| 504 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
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| 505 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
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| 506 | ) |
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| 507 | ELSE |
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| 508 | |
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| 509 | ! |
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| 510 | !-- Unstable stratification |
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| 511 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 512 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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| 513 | |
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| 514 | us_wall = kappa * vel_total / ( & |
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| 515 | LOG( zp / z0(j,i) ) - & |
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| 516 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 517 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 518 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 519 | ) |
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| 520 | ENDIF |
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| 521 | |
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| 522 | ! |
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| 523 | !-- Skip step (4) of wall_fluxes, because here rifs is already |
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| 524 | !-- available from (1) |
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| 525 | ! |
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[56] | 526 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
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[187] | 527 | !-- First interpolate the velocity (this is different from |
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| 528 | !-- subroutine wall_fluxes because fluxes in subroutine |
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| 529 | !-- wall_fluxes_e are defined at scalar locations). |
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[56] | 530 | vel_zp = 0.5 * ( a * ( u(k,j,i) + u(k,j,i+1) ) + & |
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| 531 | b * ( v(k,j,i) + v(k,j+1,i) ) + & |
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| 532 | (c1+c2) * ( w(k,j,i) + w(k-1,j,i) ) & |
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| 533 | ) |
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| 534 | |
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| 535 | IF ( rifs >= 0.0 ) THEN |
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| 536 | |
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| 537 | ! |
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| 538 | !-- Stable stratification (and neutral) |
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| 539 | wall_flux(k) = kappa * vel_zp / & |
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| 540 | ( LOG( zp/z0(j,i) ) + 5.0*rifs * ( zp-z0(j,i) ) / zp ) |
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| 541 | ELSE |
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| 542 | |
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| 543 | ! |
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| 544 | !-- Unstable stratification |
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[187] | 545 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
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| 546 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
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[56] | 547 | |
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[187] | 548 | wall_flux(k) = kappa * vel_zp / ( & |
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| 549 | LOG( zp / z0(j,i) ) - & |
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| 550 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
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| 551 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
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| 552 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
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| 553 | ) |
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[53] | 554 | ENDIF |
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[187] | 555 | wall_flux(k) = - wall_flux(k) * us_wall |
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[53] | 556 | |
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[56] | 557 | ENDDO |
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[53] | 558 | |
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[56] | 559 | END SUBROUTINE wall_fluxes_e_ij |
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| 560 | |
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| 561 | END MODULE wall_fluxes_mod |
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