1 | MODULE wall_fluxes_mod |
---|
2 | |
---|
3 | !--------------------------------------------------------------------------------! |
---|
4 | ! This file is part of PALM. |
---|
5 | ! |
---|
6 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
---|
7 | ! of the GNU General Public License as published by the Free Software Foundation, |
---|
8 | ! either version 3 of the License, or (at your option) any later version. |
---|
9 | ! |
---|
10 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
---|
11 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
---|
12 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
---|
13 | ! |
---|
14 | ! You should have received a copy of the GNU General Public License along with |
---|
15 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
---|
16 | ! |
---|
17 | ! Copyright 1997-2012 Leibniz University Hannover |
---|
18 | !--------------------------------------------------------------------------------! |
---|
19 | ! |
---|
20 | ! Current revisions: |
---|
21 | ! ----------------- |
---|
22 | ! |
---|
23 | ! |
---|
24 | ! Former revisions: |
---|
25 | ! ----------------- |
---|
26 | ! $Id: wall_fluxes.f90 1154 2013-05-10 14:43:15Z fuhrmann $ |
---|
27 | ! |
---|
28 | ! 1153 2013-05-10 14:33:08Z raasch |
---|
29 | ! code adjustments of accelerator version required by PGI 12.3 / CUDA 5.0 |
---|
30 | ! |
---|
31 | ! 1128 2013-04-12 06:19:32Z raasch |
---|
32 | ! loop index bounds in accelerator version replaced by i_left, i_right, j_south, |
---|
33 | ! j_north |
---|
34 | ! |
---|
35 | ! 1036 2012-10-22 13:43:42Z raasch |
---|
36 | ! code put under GPL (PALM 3.9) |
---|
37 | ! |
---|
38 | ! 1015 2012-09-27 09:23:24Z raasch |
---|
39 | ! accelerator version (*_acc) added |
---|
40 | ! |
---|
41 | ! 187 2008-08-06 16:25:09Z letzel |
---|
42 | ! Bugfix: Modification of the evaluation of the vertical turbulent momentum |
---|
43 | ! fluxes u'w' and v'w (see prandtl_fluxes), this requires the calculation of |
---|
44 | ! us_wall (and vel_total, u_i, v_i, ws) also in wall_fluxes_e. |
---|
45 | ! Bugfix: change definition of us_wall from 1D to 2D |
---|
46 | ! Bugfix: storage of rifs to rifs_wall in wall_fluxes_e removed |
---|
47 | ! Change: add 'minus' sign to fluxes produced by subroutine wall_fluxes_e for |
---|
48 | ! consistency with subroutine wall_fluxes |
---|
49 | ! Change: Modification of the integrated version of the profile function for |
---|
50 | ! momentum for unstable stratification |
---|
51 | ! |
---|
52 | ! Initial version (2007/03/07) |
---|
53 | ! |
---|
54 | ! Description: |
---|
55 | ! ------------ |
---|
56 | ! Calculates momentum fluxes at vertical walls assuming Monin-Obukhov |
---|
57 | ! similarity. |
---|
58 | ! Indices: usvs a=1, vsus b=1, wsvs c1=1, wsus c2=1 (other=0). |
---|
59 | ! The all-gridpoint version of wall_fluxes_e is not used so far, because |
---|
60 | ! it gives slightly different results from the ij-version for some unknown |
---|
61 | ! reason. |
---|
62 | !------------------------------------------------------------------------------! |
---|
63 | PRIVATE |
---|
64 | PUBLIC wall_fluxes, wall_fluxes_acc, wall_fluxes_e, wall_fluxes_e_acc |
---|
65 | |
---|
66 | INTERFACE wall_fluxes |
---|
67 | MODULE PROCEDURE wall_fluxes |
---|
68 | MODULE PROCEDURE wall_fluxes_ij |
---|
69 | END INTERFACE wall_fluxes |
---|
70 | |
---|
71 | INTERFACE wall_fluxes_acc |
---|
72 | MODULE PROCEDURE wall_fluxes_acc |
---|
73 | END INTERFACE wall_fluxes_acc |
---|
74 | |
---|
75 | INTERFACE wall_fluxes_e |
---|
76 | MODULE PROCEDURE wall_fluxes_e |
---|
77 | MODULE PROCEDURE wall_fluxes_e_ij |
---|
78 | END INTERFACE wall_fluxes_e |
---|
79 | |
---|
80 | INTERFACE wall_fluxes_e_acc |
---|
81 | MODULE PROCEDURE wall_fluxes_e_acc |
---|
82 | END INTERFACE wall_fluxes_e_acc |
---|
83 | |
---|
84 | CONTAINS |
---|
85 | |
---|
86 | !------------------------------------------------------------------------------! |
---|
87 | ! Call for all grid points |
---|
88 | !------------------------------------------------------------------------------! |
---|
89 | SUBROUTINE wall_fluxes( wall_flux, a, b, c1, c2, nzb_uvw_inner, & |
---|
90 | nzb_uvw_outer, wall ) |
---|
91 | |
---|
92 | USE arrays_3d |
---|
93 | USE control_parameters |
---|
94 | USE grid_variables |
---|
95 | USE indices |
---|
96 | USE statistics |
---|
97 | |
---|
98 | IMPLICIT NONE |
---|
99 | |
---|
100 | INTEGER :: i, j, k, wall_index |
---|
101 | |
---|
102 | INTEGER, DIMENSION(nysg:nyng,nxlg:nxrg) :: nzb_uvw_inner, & |
---|
103 | nzb_uvw_outer |
---|
104 | REAL :: a, b, c1, c2, h1, h2, zp |
---|
105 | REAL :: pts, pt_i, rifs, u_i, v_i, us_wall, vel_total, ws, wspts |
---|
106 | |
---|
107 | REAL, DIMENSION(nysg:nyng,nxlg:nxrg) :: wall |
---|
108 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
---|
109 | |
---|
110 | |
---|
111 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
---|
112 | wall_flux = 0.0 |
---|
113 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
---|
114 | |
---|
115 | DO i = nxl, nxr |
---|
116 | DO j = nys, nyn |
---|
117 | |
---|
118 | IF ( wall(j,i) /= 0.0 ) THEN |
---|
119 | ! |
---|
120 | !-- All subsequent variables are computed for the respective |
---|
121 | !-- location where the respective flux is defined. |
---|
122 | DO k = nzb_uvw_inner(j,i)+1, nzb_uvw_outer(j,i) |
---|
123 | |
---|
124 | ! |
---|
125 | !-- (1) Compute rifs, u_i, v_i, ws, pt' and w'pt' |
---|
126 | rifs = rif_wall(k,j,i,wall_index) |
---|
127 | |
---|
128 | u_i = a * u(k,j,i) + c1 * 0.25 * & |
---|
129 | ( u(k+1,j,i+1) + u(k+1,j,i) + u(k,j,i+1) + u(k,j,i) ) |
---|
130 | |
---|
131 | v_i = b * v(k,j,i) + c2 * 0.25 * & |
---|
132 | ( v(k+1,j+1,i) + v(k+1,j,i) + v(k,j+1,i) + v(k,j,i) ) |
---|
133 | |
---|
134 | ws = ( c1 + c2 ) * w(k,j,i) + 0.25 * ( & |
---|
135 | a * ( w(k-1,j,i-1) + w(k-1,j,i) + w(k,j,i-1) + w(k,j,i) ) & |
---|
136 | + b * ( w(k-1,j-1,i) + w(k-1,j,i) + w(k,j-1,i) + w(k,j,i) ) & |
---|
137 | ) |
---|
138 | pt_i = 0.5 * ( pt(k,j,i) + a * pt(k,j,i-1) + & |
---|
139 | b * pt(k,j-1,i) + ( c1 + c2 ) * pt(k+1,j,i) ) |
---|
140 | |
---|
141 | pts = pt_i - hom(k,1,4,0) |
---|
142 | wspts = ws * pts |
---|
143 | |
---|
144 | ! |
---|
145 | !-- (2) Compute wall-parallel absolute velocity vel_total |
---|
146 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
---|
147 | |
---|
148 | ! |
---|
149 | !-- (3) Compute wall friction velocity us_wall |
---|
150 | IF ( rifs >= 0.0 ) THEN |
---|
151 | |
---|
152 | ! |
---|
153 | !-- Stable stratification (and neutral) |
---|
154 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
---|
155 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
156 | ) |
---|
157 | ELSE |
---|
158 | |
---|
159 | ! |
---|
160 | !-- Unstable stratification |
---|
161 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
162 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
163 | |
---|
164 | us_wall = kappa * vel_total / ( & |
---|
165 | LOG( zp / z0(j,i) ) - & |
---|
166 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
167 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
168 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
169 | ) |
---|
170 | ENDIF |
---|
171 | |
---|
172 | ! |
---|
173 | !-- (4) Compute zp/L (corresponds to neutral Richardson flux |
---|
174 | !-- number rifs) |
---|
175 | rifs = -1.0 * zp * kappa * g * wspts / ( pt_i * & |
---|
176 | ( us_wall**3 + 1E-30 ) ) |
---|
177 | |
---|
178 | ! |
---|
179 | !-- Limit the value range of the Richardson numbers. |
---|
180 | !-- This is necessary for very small velocities (u,w --> 0), |
---|
181 | !-- because the absolute value of rif can then become very |
---|
182 | !-- large, which in consequence would result in very large |
---|
183 | !-- shear stresses and very small momentum fluxes (both are |
---|
184 | !-- generally unrealistic). |
---|
185 | IF ( rifs < rif_min ) rifs = rif_min |
---|
186 | IF ( rifs > rif_max ) rifs = rif_max |
---|
187 | |
---|
188 | ! |
---|
189 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
---|
190 | IF ( rifs >= 0.0 ) THEN |
---|
191 | |
---|
192 | ! |
---|
193 | !-- Stable stratification (and neutral) |
---|
194 | wall_flux(k,j,i) = kappa * & |
---|
195 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / & |
---|
196 | ( LOG( zp / z0(j,i) ) + & |
---|
197 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
198 | ) |
---|
199 | ELSE |
---|
200 | |
---|
201 | ! |
---|
202 | !-- Unstable stratification |
---|
203 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
204 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
205 | |
---|
206 | wall_flux(k,j,i) = kappa * & |
---|
207 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / ( & |
---|
208 | LOG( zp / z0(j,i) ) - & |
---|
209 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
210 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
211 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
212 | ) |
---|
213 | ENDIF |
---|
214 | wall_flux(k,j,i) = -wall_flux(k,j,i) * us_wall |
---|
215 | |
---|
216 | ! |
---|
217 | !-- store rifs for next time step |
---|
218 | rif_wall(k,j,i,wall_index) = rifs |
---|
219 | |
---|
220 | ENDDO |
---|
221 | |
---|
222 | ENDIF |
---|
223 | |
---|
224 | ENDDO |
---|
225 | ENDDO |
---|
226 | |
---|
227 | END SUBROUTINE wall_fluxes |
---|
228 | |
---|
229 | |
---|
230 | !------------------------------------------------------------------------------! |
---|
231 | ! Call for all grid points - accelerator version |
---|
232 | !------------------------------------------------------------------------------! |
---|
233 | SUBROUTINE wall_fluxes_acc( wall_flux, a, b, c1, c2, nzb_uvw_inner, & |
---|
234 | nzb_uvw_outer, wall ) |
---|
235 | |
---|
236 | USE arrays_3d |
---|
237 | USE control_parameters |
---|
238 | USE grid_variables |
---|
239 | USE indices |
---|
240 | USE statistics |
---|
241 | |
---|
242 | IMPLICIT NONE |
---|
243 | |
---|
244 | INTEGER :: i, j, k, max_outer, min_inner, wall_index |
---|
245 | |
---|
246 | INTEGER, DIMENSION(nysg:nyng,nxlg:nxrg) :: nzb_uvw_inner, & |
---|
247 | nzb_uvw_outer |
---|
248 | REAL :: a, b, c1, c2, h1, h2, zp |
---|
249 | REAL :: pts, pt_i, rifs, u_i, v_i, us_wall, vel_total, ws, wspts |
---|
250 | |
---|
251 | REAL, DIMENSION(nysg:nyng,nxlg:nxrg) :: wall |
---|
252 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
---|
253 | |
---|
254 | |
---|
255 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
---|
256 | wall_flux = 0.0 |
---|
257 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
---|
258 | |
---|
259 | min_inner = MINVAL( nzb_uvw_inner(nys:nyn,nxl:nxr) ) + 1 |
---|
260 | max_outer = MINVAL( nzb_uvw_outer(nys:nyn,nxl:nxr) ) |
---|
261 | |
---|
262 | !$acc kernels present( hom, nzb_uvw_inner, nzb_uvw_outer, pt, rif_wall ) & |
---|
263 | !$acc present( u, v, w, wall, wall_flux, z0 ) |
---|
264 | !$acc loop independent |
---|
265 | DO i = i_left, i_right |
---|
266 | DO j = j_south, j_north |
---|
267 | |
---|
268 | IF ( wall(j,i) /= 0.0 ) THEN |
---|
269 | ! |
---|
270 | !-- All subsequent variables are computed for the respective |
---|
271 | !-- location where the respective flux is defined. |
---|
272 | !$acc loop independent vector( 32 ) |
---|
273 | DO k = nzb_uvw_inner(j,i)+1, nzb_uvw_outer(j,i) |
---|
274 | |
---|
275 | ! |
---|
276 | !-- (1) Compute rifs, u_i, v_i, ws, pt' and w'pt' |
---|
277 | rifs = rif_wall(k,j,i,wall_index) |
---|
278 | |
---|
279 | u_i = a * u(k,j,i) + c1 * 0.25 * & |
---|
280 | ( u(k+1,j,i+1) + u(k+1,j,i) + u(k,j,i+1) + u(k,j,i) ) |
---|
281 | |
---|
282 | v_i = b * v(k,j,i) + c2 * 0.25 * & |
---|
283 | ( v(k+1,j+1,i) + v(k+1,j,i) + v(k,j+1,i) + v(k,j,i) ) |
---|
284 | |
---|
285 | ws = ( c1 + c2 ) * w(k,j,i) + 0.25 * ( & |
---|
286 | a * ( w(k-1,j,i-1) + w(k-1,j,i) + w(k,j,i-1) + w(k,j,i) ) & |
---|
287 | + b * ( w(k-1,j-1,i) + w(k-1,j,i) + w(k,j-1,i) + w(k,j,i) ) & |
---|
288 | ) |
---|
289 | pt_i = 0.5 * ( pt(k,j,i) + a * pt(k,j,i-1) + & |
---|
290 | b * pt(k,j-1,i) + ( c1 + c2 ) * pt(k+1,j,i) ) |
---|
291 | |
---|
292 | pts = pt_i - hom(k,1,4,0) |
---|
293 | wspts = ws * pts |
---|
294 | |
---|
295 | ! |
---|
296 | !-- (2) Compute wall-parallel absolute velocity vel_total |
---|
297 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
---|
298 | |
---|
299 | ! |
---|
300 | !-- (3) Compute wall friction velocity us_wall |
---|
301 | IF ( rifs >= 0.0 ) THEN |
---|
302 | |
---|
303 | ! |
---|
304 | !-- Stable stratification (and neutral) |
---|
305 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
---|
306 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
307 | ) |
---|
308 | ELSE |
---|
309 | |
---|
310 | ! |
---|
311 | !-- Unstable stratification |
---|
312 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
313 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
314 | |
---|
315 | us_wall = kappa * vel_total / ( & |
---|
316 | LOG( zp / z0(j,i) ) - & |
---|
317 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
318 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
319 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
320 | ) |
---|
321 | ENDIF |
---|
322 | |
---|
323 | ! |
---|
324 | !-- (4) Compute zp/L (corresponds to neutral Richardson flux |
---|
325 | !-- number rifs) |
---|
326 | rifs = -1.0 * zp * kappa * g * wspts / ( pt_i * & |
---|
327 | ( us_wall**3 + 1E-30 ) ) |
---|
328 | |
---|
329 | ! |
---|
330 | !-- Limit the value range of the Richardson numbers. |
---|
331 | !-- This is necessary for very small velocities (u,w --> 0), |
---|
332 | !-- because the absolute value of rif can then become very |
---|
333 | !-- large, which in consequence would result in very large |
---|
334 | !-- shear stresses and very small momentum fluxes (both are |
---|
335 | !-- generally unrealistic). |
---|
336 | IF ( rifs < rif_min ) rifs = rif_min |
---|
337 | IF ( rifs > rif_max ) rifs = rif_max |
---|
338 | |
---|
339 | ! |
---|
340 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
---|
341 | IF ( rifs >= 0.0 ) THEN |
---|
342 | |
---|
343 | ! |
---|
344 | !-- Stable stratification (and neutral) |
---|
345 | wall_flux(k,j,i) = kappa * & |
---|
346 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / & |
---|
347 | ( LOG( zp / z0(j,i) ) + & |
---|
348 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
349 | ) |
---|
350 | ELSE |
---|
351 | |
---|
352 | ! |
---|
353 | !-- Unstable stratification |
---|
354 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
355 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
356 | |
---|
357 | wall_flux(k,j,i) = kappa * & |
---|
358 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / ( & |
---|
359 | LOG( zp / z0(j,i) ) - & |
---|
360 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
361 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
362 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
363 | ) |
---|
364 | ENDIF |
---|
365 | wall_flux(k,j,i) = -wall_flux(k,j,i) * us_wall |
---|
366 | |
---|
367 | ! |
---|
368 | !-- store rifs for next time step |
---|
369 | rif_wall(k,j,i,wall_index) = rifs |
---|
370 | |
---|
371 | ! ENDIF |
---|
372 | |
---|
373 | ENDDO |
---|
374 | |
---|
375 | ENDIF |
---|
376 | |
---|
377 | ENDDO |
---|
378 | ENDDO |
---|
379 | !$acc end kernels |
---|
380 | |
---|
381 | END SUBROUTINE wall_fluxes_acc |
---|
382 | |
---|
383 | |
---|
384 | !------------------------------------------------------------------------------! |
---|
385 | ! Call for all grid point i,j |
---|
386 | !------------------------------------------------------------------------------! |
---|
387 | SUBROUTINE wall_fluxes_ij( i, j, nzb_w, nzt_w, wall_flux, a, b, c1, c2 ) |
---|
388 | |
---|
389 | USE arrays_3d |
---|
390 | USE control_parameters |
---|
391 | USE grid_variables |
---|
392 | USE indices |
---|
393 | USE statistics |
---|
394 | |
---|
395 | IMPLICIT NONE |
---|
396 | |
---|
397 | INTEGER :: i, j, k, nzb_w, nzt_w, wall_index |
---|
398 | REAL :: a, b, c1, c2, h1, h2, zp |
---|
399 | |
---|
400 | REAL :: pts, pt_i, rifs, u_i, v_i, us_wall, vel_total, ws, wspts |
---|
401 | |
---|
402 | REAL, DIMENSION(nzb:nzt+1) :: wall_flux |
---|
403 | |
---|
404 | |
---|
405 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
---|
406 | wall_flux = 0.0 |
---|
407 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
---|
408 | |
---|
409 | ! |
---|
410 | !-- All subsequent variables are computed for the respective location where |
---|
411 | !-- the respective flux is defined. |
---|
412 | DO k = nzb_w, nzt_w |
---|
413 | |
---|
414 | ! |
---|
415 | !-- (1) Compute rifs, u_i, v_i, ws, pt' and w'pt' |
---|
416 | rifs = rif_wall(k,j,i,wall_index) |
---|
417 | |
---|
418 | u_i = a * u(k,j,i) + c1 * 0.25 * & |
---|
419 | ( u(k+1,j,i+1) + u(k+1,j,i) + u(k,j,i+1) + u(k,j,i) ) |
---|
420 | |
---|
421 | v_i = b * v(k,j,i) + c2 * 0.25 * & |
---|
422 | ( v(k+1,j+1,i) + v(k+1,j,i) + v(k,j+1,i) + v(k,j,i) ) |
---|
423 | |
---|
424 | ws = ( c1 + c2 ) * w(k,j,i) + 0.25 * ( & |
---|
425 | a * ( w(k-1,j,i-1) + w(k-1,j,i) + w(k,j,i-1) + w(k,j,i) ) & |
---|
426 | + b * ( w(k-1,j-1,i) + w(k-1,j,i) + w(k,j-1,i) + w(k,j,i) ) & |
---|
427 | ) |
---|
428 | pt_i = 0.5 * ( pt(k,j,i) + a * pt(k,j,i-1) + b * pt(k,j-1,i) & |
---|
429 | + ( c1 + c2 ) * pt(k+1,j,i) ) |
---|
430 | |
---|
431 | pts = pt_i - hom(k,1,4,0) |
---|
432 | wspts = ws * pts |
---|
433 | |
---|
434 | ! |
---|
435 | !-- (2) Compute wall-parallel absolute velocity vel_total |
---|
436 | vel_total = SQRT( ws**2 + ( a+c1 ) * u_i**2 + ( b+c2 ) * v_i**2 ) |
---|
437 | |
---|
438 | ! |
---|
439 | !-- (3) Compute wall friction velocity us_wall |
---|
440 | IF ( rifs >= 0.0 ) THEN |
---|
441 | |
---|
442 | ! |
---|
443 | !-- Stable stratification (and neutral) |
---|
444 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
---|
445 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
446 | ) |
---|
447 | ELSE |
---|
448 | |
---|
449 | ! |
---|
450 | !-- Unstable stratification |
---|
451 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
452 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
453 | |
---|
454 | us_wall = kappa * vel_total / ( & |
---|
455 | LOG( zp / z0(j,i) ) - & |
---|
456 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
457 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
458 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
459 | ) |
---|
460 | ENDIF |
---|
461 | |
---|
462 | ! |
---|
463 | !-- (4) Compute zp/L (corresponds to neutral Richardson flux number |
---|
464 | !-- rifs) |
---|
465 | rifs = -1.0 * zp * kappa * g * wspts / ( pt_i * (us_wall**3 + 1E-30) ) |
---|
466 | |
---|
467 | ! |
---|
468 | !-- Limit the value range of the Richardson numbers. |
---|
469 | !-- This is necessary for very small velocities (u,w --> 0), because |
---|
470 | !-- the absolute value of rif can then become very large, which in |
---|
471 | !-- consequence would result in very large shear stresses and very |
---|
472 | !-- small momentum fluxes (both are generally unrealistic). |
---|
473 | IF ( rifs < rif_min ) rifs = rif_min |
---|
474 | IF ( rifs > rif_max ) rifs = rif_max |
---|
475 | |
---|
476 | ! |
---|
477 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
---|
478 | IF ( rifs >= 0.0 ) THEN |
---|
479 | |
---|
480 | ! |
---|
481 | !-- Stable stratification (and neutral) |
---|
482 | wall_flux(k) = kappa * & |
---|
483 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / & |
---|
484 | ( LOG( zp / z0(j,i) ) + & |
---|
485 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
486 | ) |
---|
487 | ELSE |
---|
488 | |
---|
489 | ! |
---|
490 | !-- Unstable stratification |
---|
491 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
492 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
493 | |
---|
494 | wall_flux(k) = kappa * & |
---|
495 | ( a*u(k,j,i) + b*v(k,j,i) + (c1+c2)*w(k,j,i) ) / ( & |
---|
496 | LOG( zp / z0(j,i) ) - & |
---|
497 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
498 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
499 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
500 | ) |
---|
501 | ENDIF |
---|
502 | wall_flux(k) = -wall_flux(k) * us_wall |
---|
503 | |
---|
504 | ! |
---|
505 | !-- store rifs for next time step |
---|
506 | rif_wall(k,j,i,wall_index) = rifs |
---|
507 | |
---|
508 | ENDDO |
---|
509 | |
---|
510 | END SUBROUTINE wall_fluxes_ij |
---|
511 | |
---|
512 | |
---|
513 | |
---|
514 | !------------------------------------------------------------------------------! |
---|
515 | ! Call for all grid points |
---|
516 | !------------------------------------------------------------------------------! |
---|
517 | SUBROUTINE wall_fluxes_e( wall_flux, a, b, c1, c2, wall ) |
---|
518 | |
---|
519 | !------------------------------------------------------------------------------! |
---|
520 | ! Description: |
---|
521 | ! ------------ |
---|
522 | ! Calculates momentum fluxes at vertical walls for routine production_e |
---|
523 | ! assuming Monin-Obukhov similarity. |
---|
524 | ! Indices: usvs a=1, vsus b=1, wsvs c1=1, wsus c2=1 (other=0). |
---|
525 | !------------------------------------------------------------------------------! |
---|
526 | |
---|
527 | USE arrays_3d |
---|
528 | USE control_parameters |
---|
529 | USE grid_variables |
---|
530 | USE indices |
---|
531 | USE statistics |
---|
532 | |
---|
533 | IMPLICIT NONE |
---|
534 | |
---|
535 | INTEGER :: i, j, k, kk, wall_index |
---|
536 | REAL :: a, b, c1, c2, h1, h2, u_i, v_i, us_wall, vel_total, vel_zp, & |
---|
537 | ws, zp |
---|
538 | |
---|
539 | REAL :: rifs |
---|
540 | |
---|
541 | REAL, DIMENSION(nysg:nyng,nxlg:nxrg) :: wall |
---|
542 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
---|
543 | |
---|
544 | |
---|
545 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
---|
546 | wall_flux = 0.0 |
---|
547 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
---|
548 | |
---|
549 | DO i = nxl, nxr |
---|
550 | DO j = nys, nyn |
---|
551 | |
---|
552 | IF ( wall(j,i) /= 0.0 ) THEN |
---|
553 | ! |
---|
554 | !-- All subsequent variables are computed for scalar locations. |
---|
555 | DO k = nzb_diff_s_inner(j,i)-1, nzb_diff_s_outer(j,i)-2 |
---|
556 | ! |
---|
557 | !-- (1) Compute rifs, u_i, v_i, and ws |
---|
558 | IF ( k == nzb_diff_s_inner(j,i)-1 ) THEN |
---|
559 | kk = nzb_diff_s_inner(j,i)-1 |
---|
560 | ELSE |
---|
561 | kk = k-1 |
---|
562 | ENDIF |
---|
563 | rifs = 0.5 * ( rif_wall(k,j,i,wall_index) + & |
---|
564 | a * rif_wall(k,j,i+1,1) + b * rif_wall(k,j+1,i,2) + & |
---|
565 | c1 * rif_wall(kk,j,i,3) + c2 * rif_wall(kk,j,i,4) & |
---|
566 | ) |
---|
567 | |
---|
568 | u_i = 0.5 * ( u(k,j,i) + u(k,j,i+1) ) |
---|
569 | v_i = 0.5 * ( v(k,j,i) + v(k,j+1,i) ) |
---|
570 | ws = 0.5 * ( w(k,j,i) + w(k-1,j,i) ) |
---|
571 | ! |
---|
572 | !-- (2) Compute wall-parallel absolute velocity vel_total and |
---|
573 | !-- interpolate appropriate velocity component vel_zp. |
---|
574 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
---|
575 | vel_zp = 0.5 * ( a * u_i + b * v_i + (c1+c2) * ws ) |
---|
576 | ! |
---|
577 | !-- (3) Compute wall friction velocity us_wall |
---|
578 | IF ( rifs >= 0.0 ) THEN |
---|
579 | |
---|
580 | ! |
---|
581 | !-- Stable stratification (and neutral) |
---|
582 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
---|
583 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
584 | ) |
---|
585 | ELSE |
---|
586 | |
---|
587 | ! |
---|
588 | !-- Unstable stratification |
---|
589 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
590 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
591 | |
---|
592 | us_wall = kappa * vel_total / ( & |
---|
593 | LOG( zp / z0(j,i) ) - & |
---|
594 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
595 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
596 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
597 | ) |
---|
598 | ENDIF |
---|
599 | |
---|
600 | ! |
---|
601 | !-- Skip step (4) of wall_fluxes, because here rifs is already |
---|
602 | !-- available from (1) |
---|
603 | ! |
---|
604 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
---|
605 | |
---|
606 | IF ( rifs >= 0.0 ) THEN |
---|
607 | |
---|
608 | ! |
---|
609 | !-- Stable stratification (and neutral) |
---|
610 | wall_flux(k,j,i) = kappa * vel_zp / & |
---|
611 | ( LOG( zp/z0(j,i) ) + 5.0*rifs * ( zp-z0(j,i) ) / zp ) |
---|
612 | ELSE |
---|
613 | |
---|
614 | ! |
---|
615 | !-- Unstable stratification |
---|
616 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
617 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
618 | |
---|
619 | wall_flux(k,j,i) = kappa * vel_zp / ( & |
---|
620 | LOG( zp / z0(j,i) ) - & |
---|
621 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
622 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
623 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
624 | ) |
---|
625 | ENDIF |
---|
626 | wall_flux(k,j,i) = - wall_flux(k,j,i) * us_wall |
---|
627 | |
---|
628 | ENDDO |
---|
629 | |
---|
630 | ENDIF |
---|
631 | |
---|
632 | ENDDO |
---|
633 | ENDDO |
---|
634 | |
---|
635 | END SUBROUTINE wall_fluxes_e |
---|
636 | |
---|
637 | |
---|
638 | !------------------------------------------------------------------------------! |
---|
639 | ! Call for all grid points - accelerator version |
---|
640 | !------------------------------------------------------------------------------! |
---|
641 | SUBROUTINE wall_fluxes_e_acc( wall_flux, a, b, c1, c2, wall ) |
---|
642 | |
---|
643 | !------------------------------------------------------------------------------! |
---|
644 | ! Description: |
---|
645 | ! ------------ |
---|
646 | ! Calculates momentum fluxes at vertical walls for routine production_e |
---|
647 | ! assuming Monin-Obukhov similarity. |
---|
648 | ! Indices: usvs a=1, vsus b=1, wsvs c1=1, wsus c2=1 (other=0). |
---|
649 | !------------------------------------------------------------------------------! |
---|
650 | |
---|
651 | USE arrays_3d |
---|
652 | USE control_parameters |
---|
653 | USE grid_variables |
---|
654 | USE indices |
---|
655 | USE statistics |
---|
656 | |
---|
657 | IMPLICIT NONE |
---|
658 | |
---|
659 | INTEGER :: i, j, k, kk, max_outer, min_inner, wall_index |
---|
660 | REAL :: a, b, c1, c2, h1, h2, u_i, v_i, us_wall, vel_total, vel_zp, & |
---|
661 | ws, zp |
---|
662 | |
---|
663 | REAL :: rifs |
---|
664 | |
---|
665 | REAL, DIMENSION(nysg:nyng,nxlg:nxrg) :: wall |
---|
666 | REAL, DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: wall_flux |
---|
667 | |
---|
668 | |
---|
669 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
---|
670 | wall_flux = 0.0 |
---|
671 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
---|
672 | |
---|
673 | min_inner = MINVAL( nzb_diff_s_inner(nys:nyn,nxl:nxr) ) - 1 |
---|
674 | max_outer = MAXVAL( nzb_diff_s_outer(nys:nyn,nxl:nxr) ) - 2 |
---|
675 | |
---|
676 | !$acc kernels present( nzb_diff_s_inner, nzb_diff_s_outer, pt, rif_wall ) & |
---|
677 | !$acc present( u, v, w, wall, wall_flux, z0 ) |
---|
678 | !$acc loop |
---|
679 | DO i = i_left, i_right |
---|
680 | DO j = j_south, j_north |
---|
681 | !$acc loop vector(32) |
---|
682 | DO k = min_inner, max_outer |
---|
683 | ! |
---|
684 | !-- All subsequent variables are computed for scalar locations |
---|
685 | IF ( k >= nzb_diff_s_inner(j,i)-1 .AND. & |
---|
686 | k <= nzb_diff_s_outer(j,i)-2 .AND. wall(j,i) /= 0.0 ) THEN |
---|
687 | ! |
---|
688 | !-- (1) Compute rifs, u_i, v_i, and ws |
---|
689 | IF ( k == nzb_diff_s_inner(j,i)-1 ) THEN |
---|
690 | kk = nzb_diff_s_inner(j,i)-1 |
---|
691 | ELSE |
---|
692 | kk = k-1 |
---|
693 | ENDIF |
---|
694 | rifs = 0.5 * ( rif_wall(k,j,i,wall_index) + & |
---|
695 | a * rif_wall(k,j,i+1,1) + b * rif_wall(k,j+1,i,2) + & |
---|
696 | c1 * rif_wall(kk,j,i,3) + c2 * rif_wall(kk,j,i,4) & |
---|
697 | ) |
---|
698 | |
---|
699 | u_i = 0.5 * ( u(k,j,i) + u(k,j,i+1) ) |
---|
700 | v_i = 0.5 * ( v(k,j,i) + v(k,j+1,i) ) |
---|
701 | ws = 0.5 * ( w(k,j,i) + w(k-1,j,i) ) |
---|
702 | ! |
---|
703 | !-- (2) Compute wall-parallel absolute velocity vel_total and |
---|
704 | !-- interpolate appropriate velocity component vel_zp. |
---|
705 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
---|
706 | vel_zp = 0.5 * ( a * u_i + b * v_i + (c1+c2) * ws ) |
---|
707 | ! |
---|
708 | !-- (3) Compute wall friction velocity us_wall |
---|
709 | IF ( rifs >= 0.0 ) THEN |
---|
710 | |
---|
711 | ! |
---|
712 | !-- Stable stratification (and neutral) |
---|
713 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
---|
714 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
715 | ) |
---|
716 | ELSE |
---|
717 | |
---|
718 | ! |
---|
719 | !-- Unstable stratification |
---|
720 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
721 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
722 | |
---|
723 | us_wall = kappa * vel_total / ( & |
---|
724 | LOG( zp / z0(j,i) ) - & |
---|
725 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
726 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
727 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
728 | ) |
---|
729 | ENDIF |
---|
730 | |
---|
731 | ! |
---|
732 | !-- Skip step (4) of wall_fluxes, because here rifs is already |
---|
733 | !-- available from (1) |
---|
734 | ! |
---|
735 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
---|
736 | |
---|
737 | IF ( rifs >= 0.0 ) THEN |
---|
738 | |
---|
739 | ! |
---|
740 | !-- Stable stratification (and neutral) |
---|
741 | wall_flux(k,j,i) = kappa * vel_zp / & |
---|
742 | ( LOG( zp/z0(j,i) ) + 5.0*rifs * ( zp-z0(j,i) ) / zp ) |
---|
743 | ELSE |
---|
744 | |
---|
745 | ! |
---|
746 | !-- Unstable stratification |
---|
747 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
748 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
749 | |
---|
750 | wall_flux(k,j,i) = kappa * vel_zp / ( & |
---|
751 | LOG( zp / z0(j,i) ) - & |
---|
752 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
753 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
754 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
755 | ) |
---|
756 | ENDIF |
---|
757 | wall_flux(k,j,i) = - wall_flux(k,j,i) * us_wall |
---|
758 | |
---|
759 | ENDIF |
---|
760 | |
---|
761 | ENDDO |
---|
762 | ENDDO |
---|
763 | ENDDO |
---|
764 | !$acc end kernels |
---|
765 | |
---|
766 | END SUBROUTINE wall_fluxes_e_acc |
---|
767 | |
---|
768 | |
---|
769 | !------------------------------------------------------------------------------! |
---|
770 | ! Call for grid point i,j |
---|
771 | !------------------------------------------------------------------------------! |
---|
772 | SUBROUTINE wall_fluxes_e_ij( i, j, nzb_w, nzt_w, wall_flux, a, b, c1, c2 ) |
---|
773 | |
---|
774 | USE arrays_3d |
---|
775 | USE control_parameters |
---|
776 | USE grid_variables |
---|
777 | USE indices |
---|
778 | USE statistics |
---|
779 | |
---|
780 | IMPLICIT NONE |
---|
781 | |
---|
782 | INTEGER :: i, j, k, kk, nzb_w, nzt_w, wall_index |
---|
783 | REAL :: a, b, c1, c2, h1, h2, u_i, v_i, us_wall, vel_total, vel_zp, & |
---|
784 | ws, zp |
---|
785 | |
---|
786 | REAL :: rifs |
---|
787 | |
---|
788 | REAL, DIMENSION(nzb:nzt+1) :: wall_flux |
---|
789 | |
---|
790 | |
---|
791 | zp = 0.5 * ( (a+c1) * dy + (b+c2) * dx ) |
---|
792 | wall_flux = 0.0 |
---|
793 | wall_index = NINT( a+ 2*b + 3*c1 + 4*c2 ) |
---|
794 | |
---|
795 | ! |
---|
796 | !-- All subsequent variables are computed for scalar locations. |
---|
797 | DO k = nzb_w, nzt_w |
---|
798 | |
---|
799 | ! |
---|
800 | !-- (1) Compute rifs, u_i, v_i, and ws |
---|
801 | IF ( k == nzb_w ) THEN |
---|
802 | kk = nzb_w |
---|
803 | ELSE |
---|
804 | kk = k-1 |
---|
805 | ENDIF |
---|
806 | rifs = 0.5 * ( rif_wall(k,j,i,wall_index) + & |
---|
807 | a * rif_wall(k,j,i+1,1) + b * rif_wall(k,j+1,i,2) + & |
---|
808 | c1 * rif_wall(kk,j,i,3) + c2 * rif_wall(kk,j,i,4) & |
---|
809 | ) |
---|
810 | |
---|
811 | u_i = 0.5 * ( u(k,j,i) + u(k,j,i+1) ) |
---|
812 | v_i = 0.5 * ( v(k,j,i) + v(k,j+1,i) ) |
---|
813 | ws = 0.5 * ( w(k,j,i) + w(k-1,j,i) ) |
---|
814 | ! |
---|
815 | !-- (2) Compute wall-parallel absolute velocity vel_total and |
---|
816 | !-- interpolate appropriate velocity component vel_zp. |
---|
817 | vel_total = SQRT( ws**2 + (a+c1) * u_i**2 + (b+c2) * v_i**2 ) |
---|
818 | vel_zp = 0.5 * ( a * u_i + b * v_i + (c1+c2) * ws ) |
---|
819 | ! |
---|
820 | !-- (3) Compute wall friction velocity us_wall |
---|
821 | IF ( rifs >= 0.0 ) THEN |
---|
822 | |
---|
823 | ! |
---|
824 | !-- Stable stratification (and neutral) |
---|
825 | us_wall = kappa * vel_total / ( LOG( zp / z0(j,i) ) + & |
---|
826 | 5.0 * rifs * ( zp - z0(j,i) ) / zp & |
---|
827 | ) |
---|
828 | ELSE |
---|
829 | |
---|
830 | ! |
---|
831 | !-- Unstable stratification |
---|
832 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
833 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
834 | |
---|
835 | us_wall = kappa * vel_total / ( & |
---|
836 | LOG( zp / z0(j,i) ) - & |
---|
837 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
838 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
839 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
840 | ) |
---|
841 | ENDIF |
---|
842 | |
---|
843 | ! |
---|
844 | !-- Skip step (4) of wall_fluxes, because here rifs is already |
---|
845 | !-- available from (1) |
---|
846 | ! |
---|
847 | !-- (5) Compute wall_flux (u'v', v'u', w'v', or w'u') |
---|
848 | !-- First interpolate the velocity (this is different from |
---|
849 | !-- subroutine wall_fluxes because fluxes in subroutine |
---|
850 | !-- wall_fluxes_e are defined at scalar locations). |
---|
851 | vel_zp = 0.5 * ( a * ( u(k,j,i) + u(k,j,i+1) ) + & |
---|
852 | b * ( v(k,j,i) + v(k,j+1,i) ) + & |
---|
853 | (c1+c2) * ( w(k,j,i) + w(k-1,j,i) ) & |
---|
854 | ) |
---|
855 | |
---|
856 | IF ( rifs >= 0.0 ) THEN |
---|
857 | |
---|
858 | ! |
---|
859 | !-- Stable stratification (and neutral) |
---|
860 | wall_flux(k) = kappa * vel_zp / & |
---|
861 | ( LOG( zp/z0(j,i) ) + 5.0*rifs * ( zp-z0(j,i) ) / zp ) |
---|
862 | ELSE |
---|
863 | |
---|
864 | ! |
---|
865 | !-- Unstable stratification |
---|
866 | h1 = SQRT( SQRT( 1.0 - 16.0 * rifs ) ) |
---|
867 | h2 = SQRT( SQRT( 1.0 - 16.0 * rifs * z0(j,i) / zp ) ) |
---|
868 | |
---|
869 | wall_flux(k) = kappa * vel_zp / ( & |
---|
870 | LOG( zp / z0(j,i) ) - & |
---|
871 | LOG( ( 1.0 + h1 )**2 * ( 1.0 + h1**2 ) / ( & |
---|
872 | ( 1.0 + h2 )**2 * ( 1.0 + h2**2 ) ) ) + & |
---|
873 | 2.0 * ( ATAN( h1 ) - ATAN( h2 ) ) & |
---|
874 | ) |
---|
875 | ENDIF |
---|
876 | wall_flux(k) = - wall_flux(k) * us_wall |
---|
877 | |
---|
878 | ENDDO |
---|
879 | |
---|
880 | END SUBROUTINE wall_fluxes_e_ij |
---|
881 | |
---|
882 | END MODULE wall_fluxes_mod |
---|