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