[1] | 1 | SUBROUTINE pres |
---|
| 2 | |
---|
| 3 | !------------------------------------------------------------------------------! |
---|
| 4 | ! Actual revisions: |
---|
| 5 | ! ----------------- |
---|
| 6 | ! |
---|
| 7 | ! |
---|
| 8 | ! Former revisions: |
---|
| 9 | ! ----------------- |
---|
[3] | 10 | ! $Id: pres.f90 73 2007-03-20 08:33:14Z raasch $ |
---|
| 11 | ! RCS Log replace by Id keyword, revision history cleaned up |
---|
| 12 | ! |
---|
[1] | 13 | ! Revision 1.25 2006/04/26 13:26:12 raasch |
---|
| 14 | ! OpenMP optimization (+localsum, threadsum) |
---|
| 15 | ! |
---|
| 16 | ! Revision 1.1 1997/07/24 11:24:44 raasch |
---|
| 17 | ! Initial revision |
---|
| 18 | ! |
---|
| 19 | ! |
---|
| 20 | ! Description: |
---|
| 21 | ! ------------ |
---|
| 22 | ! Compute the divergence of the provisional velocity field. Solve the Poisson |
---|
| 23 | ! equation for the perturbation pressure. Compute the final velocities using |
---|
| 24 | ! this perturbation pressure. Compute the remaining divergence. |
---|
| 25 | !------------------------------------------------------------------------------! |
---|
| 26 | |
---|
| 27 | USE arrays_3d |
---|
| 28 | USE constants |
---|
| 29 | USE control_parameters |
---|
| 30 | USE cpulog |
---|
| 31 | USE grid_variables |
---|
| 32 | USE indices |
---|
| 33 | USE interfaces |
---|
| 34 | USE pegrid |
---|
| 35 | USE poisfft_mod |
---|
| 36 | USE poisfft_hybrid_mod |
---|
| 37 | USE statistics |
---|
| 38 | |
---|
| 39 | IMPLICIT NONE |
---|
| 40 | |
---|
| 41 | INTEGER :: i, j, k, sr |
---|
| 42 | |
---|
| 43 | REAL :: localsum, threadsum |
---|
| 44 | |
---|
| 45 | REAL, DIMENSION(1:2) :: volume_flow_l, volume_flow_offset |
---|
| 46 | |
---|
| 47 | |
---|
| 48 | CALL cpu_log( log_point(8), 'pres', 'start' ) |
---|
| 49 | |
---|
| 50 | ! |
---|
| 51 | !-- Multigrid method needs additional grid points for the divergence array |
---|
| 52 | IF ( psolver == 'multigrid' ) THEN |
---|
| 53 | DEALLOCATE( d ) |
---|
| 54 | ALLOCATE( d(nzb:nzt+1,nys-1:nyn+1,nxl-1:nxr+1) ) |
---|
| 55 | ENDIF |
---|
| 56 | |
---|
| 57 | ! |
---|
| 58 | !-- Compute the divergence of the provisional velocity field. |
---|
| 59 | CALL cpu_log( log_point_s(1), 'divergence', 'start' ) |
---|
| 60 | |
---|
| 61 | IF ( psolver == 'multigrid' ) THEN |
---|
| 62 | !$OMP PARALLEL DO SCHEDULE( STATIC ) |
---|
| 63 | DO i = nxl-1, nxr+1 |
---|
| 64 | DO j = nys-1, nyn+1 |
---|
| 65 | DO k = nzb, nzt+1 |
---|
| 66 | d(k,j,i) = 0.0 |
---|
| 67 | ENDDO |
---|
| 68 | ENDDO |
---|
| 69 | ENDDO |
---|
| 70 | ELSE |
---|
| 71 | !$OMP PARALLEL DO SCHEDULE( STATIC ) |
---|
| 72 | DO i = nxl, nxra |
---|
| 73 | DO j = nys, nyna |
---|
| 74 | DO k = nzb+1, nzta |
---|
| 75 | d(k,j,i) = 0.0 |
---|
| 76 | ENDDO |
---|
| 77 | ENDDO |
---|
| 78 | ENDDO |
---|
| 79 | ENDIF |
---|
| 80 | |
---|
| 81 | localsum = 0.0 |
---|
| 82 | threadsum = 0.0 |
---|
| 83 | |
---|
| 84 | #if defined( __ibm ) |
---|
| 85 | !$OMP PARALLEL PRIVATE (i,j,k) FIRSTPRIVATE(threadsum) REDUCTION(+:localsum) |
---|
| 86 | !$OMP DO SCHEDULE( STATIC ) |
---|
| 87 | DO i = nxl, nxr |
---|
| 88 | DO j = nys, nyn |
---|
| 89 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 90 | d(k,j,i) = ( u(k,j,i+1) - u(k,j,i) ) * ddx + & |
---|
| 91 | ( v(k,j+1,i) - v(k,j,i) ) * ddy + & |
---|
| 92 | ( w(k,j,i) - w(k-1,j,i) ) * ddzw(k) |
---|
| 93 | ENDDO |
---|
| 94 | ! |
---|
| 95 | !-- Additional pressure boundary condition at the bottom boundary for |
---|
| 96 | !-- inhomogeneous Prandtl layer heat fluxes and temperatures, respectively |
---|
| 97 | !-- dp/dz = -(dtau13/dx + dtau23/dy) + g*pt'/pt0. |
---|
| 98 | !-- This condition must not be applied at the start of a run, because then |
---|
| 99 | !-- flow_statistics has not yet been called and thus sums = 0. |
---|
| 100 | IF ( ibc_p_b == 2 .AND. sums(nzb+1,4) /= 0.0 ) THEN |
---|
| 101 | k = nzb_s_inner(j,i) |
---|
| 102 | d(k+1,j,i) = d(k+1,j,i) + ( & |
---|
| 103 | ( usws(j,i+1) - usws(j,i) ) * ddx & |
---|
| 104 | + ( vsws(j+1,i) - vsws(j,i) ) * ddy & |
---|
| 105 | - g * ( pt(k+1,j,i) - sums(k+1,4) ) / & |
---|
| 106 | sums(k+1,4) & |
---|
| 107 | ) * ddzw(k+1) |
---|
| 108 | ENDIF |
---|
| 109 | |
---|
| 110 | ! |
---|
| 111 | !-- Compute possible PE-sum of divergences for flow_statistics |
---|
| 112 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 113 | threadsum = threadsum + ABS( d(k,j,i) ) |
---|
| 114 | ENDDO |
---|
| 115 | |
---|
| 116 | ! |
---|
| 117 | !-- Velocity corrections are made with Euler step size. Right hand side |
---|
| 118 | !-- of Poisson equation has to be set appropriately |
---|
| 119 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 120 | d(k,j,i) = d(k,j,i) / dt_3d |
---|
| 121 | ENDDO |
---|
| 122 | |
---|
| 123 | ENDDO |
---|
| 124 | ENDDO |
---|
| 125 | |
---|
| 126 | localsum = localsum + threadsum |
---|
| 127 | !$OMP END PARALLEL |
---|
| 128 | #else |
---|
| 129 | IF ( ibc_p_b == 2 .AND. sums(nzb+1,4) /= 0.0 ) THEN |
---|
| 130 | !$OMP PARALLEL PRIVATE (i,j,k) |
---|
| 131 | !$OMP DO SCHEDULE( STATIC ) |
---|
| 132 | DO i = nxl, nxr |
---|
| 133 | DO j = nys, nyn |
---|
| 134 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 135 | d(k,j,i) = ( u(k,j,i+1) - u(k,j,i) ) * ddx + & |
---|
| 136 | ( v(k,j+1,i) - v(k,j,i) ) * ddy + & |
---|
| 137 | ( w(k,j,i) - w(k-1,j,i) ) * ddzw(k) |
---|
| 138 | ENDDO |
---|
| 139 | ENDDO |
---|
| 140 | ! |
---|
| 141 | !-- Additional pressure boundary condition at the bottom boundary for |
---|
| 142 | !-- inhomogeneous Prandtl layer heat fluxes and temperatures, respectively |
---|
| 143 | !-- dp/dz = -(dtau13/dx + dtau23/dy) + g*pt'/pt0. |
---|
| 144 | !-- This condition must not be applied at the start of a run, because then |
---|
| 145 | !-- flow_statistics has not yet been called and thus sums = 0. |
---|
| 146 | DO j = nys, nyn |
---|
| 147 | k = nzb_s_inner(j,i) |
---|
| 148 | d(k+1,j,i) = d(k+1,j,i) + ( & |
---|
| 149 | ( usws(j,i+1) - usws(j,i) ) * ddx & |
---|
| 150 | + ( vsws(j+1,i) - vsws(j,i) ) * ddy & |
---|
| 151 | - g * ( pt(k+1,j,i) - sums(k+1,4) ) / & |
---|
| 152 | sums(k+1,4) & |
---|
| 153 | ) * ddzw(k+1) |
---|
| 154 | ENDDO |
---|
| 155 | ENDDO |
---|
| 156 | !$OMP END PARALLEL |
---|
| 157 | |
---|
| 158 | ELSE |
---|
| 159 | |
---|
| 160 | !$OMP PARALLEL PRIVATE (i,j,k) |
---|
| 161 | !$OMP DO SCHEDULE( STATIC ) |
---|
| 162 | DO i = nxl, nxr |
---|
| 163 | DO j = nys, nyn |
---|
| 164 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 165 | d(k,j,i) = ( u(k,j,i+1) - u(k,j,i) ) * ddx + & |
---|
| 166 | ( v(k,j+1,i) - v(k,j,i) ) * ddy + & |
---|
| 167 | ( w(k,j,i) - w(k-1,j,i) ) * ddzw(k) |
---|
| 168 | ENDDO |
---|
| 169 | ENDDO |
---|
| 170 | ENDDO |
---|
| 171 | !$OMP END PARALLEL |
---|
| 172 | |
---|
| 173 | ENDIF |
---|
| 174 | |
---|
| 175 | ! |
---|
| 176 | !-- Compute possible PE-sum of divergences for flow_statistics |
---|
| 177 | !$OMP PARALLEL PRIVATE (i,j,k) FIRSTPRIVATE(threadsum) REDUCTION(+:localsum) |
---|
| 178 | !$OMP DO SCHEDULE( STATIC ) |
---|
| 179 | DO i = nxl, nxr |
---|
| 180 | DO j = nys, nyn |
---|
| 181 | DO k = nzb+1, nzt |
---|
| 182 | threadsum = threadsum + ABS( d(k,j,i) ) |
---|
| 183 | ENDDO |
---|
| 184 | ENDDO |
---|
| 185 | ENDDO |
---|
| 186 | localsum = localsum + threadsum |
---|
| 187 | !$OMP END PARALLEL |
---|
| 188 | |
---|
| 189 | ! |
---|
| 190 | !-- Velocity corrections are made with Euler step size. Right hand side |
---|
| 191 | !-- of Poisson equation has to be set appropriately |
---|
| 192 | !$OMP DO SCHEDULE( STATIC ) |
---|
| 193 | DO i = nxl, nxr |
---|
| 194 | DO j = nys, nyn |
---|
| 195 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 196 | d(k,j,i) = d(k,j,i) / dt_3d |
---|
| 197 | ENDDO |
---|
| 198 | ENDDO |
---|
| 199 | ENDDO |
---|
| 200 | #endif |
---|
| 201 | |
---|
| 202 | ! |
---|
| 203 | !-- For completeness, set the divergence sum of all statistic regions to those |
---|
| 204 | !-- of the total domain |
---|
| 205 | sums_divold_l(0:statistic_regions) = localsum |
---|
| 206 | |
---|
| 207 | ! |
---|
| 208 | !-- Determine absolute minimum/maximum (only for test cases, therefore as |
---|
| 209 | !-- comment line) |
---|
| 210 | ! CALL global_min_max( nzb+1, nzt, nys, nyn, nxl, nxr, d, 'abs', divmax, & |
---|
| 211 | ! divmax_ijk ) |
---|
| 212 | |
---|
| 213 | CALL cpu_log( log_point_s(1), 'divergence', 'stop' ) |
---|
| 214 | |
---|
| 215 | ! |
---|
| 216 | !-- Compute the pressure perturbation solving the Poisson equation |
---|
| 217 | IF ( psolver(1:7) == 'poisfft' ) THEN |
---|
| 218 | |
---|
| 219 | ! |
---|
| 220 | !-- Enlarge the size of tend, used as a working array for the transpositions |
---|
| 221 | IF ( nxra > nxr .OR. nyna > nyn .OR. nza > nz ) THEN |
---|
| 222 | DEALLOCATE( tend ) |
---|
| 223 | ALLOCATE( tend(1:nza,nys:nyna,nxl:nxra) ) |
---|
| 224 | ENDIF |
---|
| 225 | |
---|
| 226 | ! |
---|
| 227 | !-- Solve Poisson equation via FFT and solution of tridiagonal matrices |
---|
| 228 | IF ( psolver == 'poisfft' ) THEN |
---|
| 229 | ! |
---|
| 230 | !-- Solver for 2d-decomposition |
---|
| 231 | CALL poisfft( d, tend ) |
---|
| 232 | ELSEIF ( psolver == 'poisfft_hybrid' ) THEN |
---|
| 233 | ! |
---|
| 234 | !-- Solver for 1d-decomposition (using MPI and OpenMP). |
---|
| 235 | !-- The old hybrid-solver is still included here, as long as there |
---|
| 236 | !-- are some optimization problems in poisfft |
---|
| 237 | CALL poisfft_hybrid( d ) |
---|
| 238 | ENDIF |
---|
| 239 | |
---|
| 240 | ! |
---|
| 241 | !-- Resize tend to its normal size |
---|
| 242 | IF ( nxra > nxr .OR. nyna > nyn .OR. nza > nz ) THEN |
---|
| 243 | DEALLOCATE( tend ) |
---|
| 244 | ALLOCATE( tend(nzb:nzt+1,nys-1:nyn+1,nxl-1:nxr+1) ) |
---|
| 245 | ENDIF |
---|
| 246 | |
---|
| 247 | ! |
---|
| 248 | !-- Store computed perturbation pressure and set boundary condition in |
---|
| 249 | !-- z-direction |
---|
| 250 | !$OMP PARALLEL DO |
---|
| 251 | DO i = nxl, nxr |
---|
| 252 | DO j = nys, nyn |
---|
| 253 | DO k = nzb+1, nzt |
---|
| 254 | tend(k,j,i) = d(k,j,i) |
---|
| 255 | ENDDO |
---|
| 256 | ENDDO |
---|
| 257 | ENDDO |
---|
| 258 | |
---|
| 259 | ! |
---|
| 260 | !-- Bottom boundary: |
---|
| 261 | !-- This condition is only required for internal output. The pressure |
---|
| 262 | !-- gradient (dp(nzb+1)-dp(nzb))/dz is not used anywhere else. |
---|
| 263 | IF ( ibc_p_b == 1 ) THEN |
---|
| 264 | ! |
---|
| 265 | !-- Neumann (dp/dz = 0) |
---|
| 266 | !$OMP PARALLEL DO |
---|
| 267 | DO i = nxl-1, nxr+1 |
---|
| 268 | DO j = nys-1, nyn+1 |
---|
| 269 | tend(nzb_s_inner(j,i),j,i) = tend(nzb_s_inner(j,i)+1,j,i) |
---|
| 270 | ENDDO |
---|
| 271 | ENDDO |
---|
| 272 | |
---|
| 273 | ELSEIF ( ibc_p_b == 2 ) THEN |
---|
| 274 | ! |
---|
| 275 | !-- Neumann condition for inhomogeneous surfaces, |
---|
| 276 | !-- here currently still in the form of a zero gradient. Actually |
---|
| 277 | !-- dp/dz = -(dtau13/dx + dtau23/dy) + g*pt'/pt0 would have to be used for |
---|
| 278 | !-- the computation (cf. above: computation of divergences). |
---|
| 279 | !$OMP PARALLEL DO |
---|
| 280 | DO i = nxl-1, nxr+1 |
---|
| 281 | DO j = nys-1, nyn+1 |
---|
| 282 | tend(nzb_s_inner(j,i),j,i) = tend(nzb_s_inner(j,i)+1,j,i) |
---|
| 283 | ENDDO |
---|
| 284 | ENDDO |
---|
| 285 | |
---|
| 286 | ELSE |
---|
| 287 | ! |
---|
| 288 | !-- Dirichlet |
---|
| 289 | !$OMP PARALLEL DO |
---|
| 290 | DO i = nxl-1, nxr+1 |
---|
| 291 | DO j = nys-1, nyn+1 |
---|
| 292 | tend(nzb_s_inner(j,i),j,i) = 0.0 |
---|
| 293 | ENDDO |
---|
| 294 | ENDDO |
---|
| 295 | |
---|
| 296 | ENDIF |
---|
| 297 | |
---|
| 298 | ! |
---|
| 299 | !-- Top boundary |
---|
| 300 | IF ( ibc_p_t == 1 ) THEN |
---|
| 301 | ! |
---|
| 302 | !-- Neumann |
---|
| 303 | !$OMP PARALLEL DO |
---|
| 304 | DO i = nxl-1, nxr+1 |
---|
| 305 | DO j = nys-1, nyn+1 |
---|
| 306 | tend(nzt+1,j,i) = tend(nzt,j,i) |
---|
| 307 | ENDDO |
---|
| 308 | ENDDO |
---|
| 309 | |
---|
| 310 | ELSE |
---|
| 311 | ! |
---|
| 312 | !-- Dirichlet |
---|
| 313 | !$OMP PARALLEL DO |
---|
| 314 | DO i = nxl-1, nxr+1 |
---|
| 315 | DO j = nys-1, nyn+1 |
---|
| 316 | tend(nzt+1,j,i) = 0.0 |
---|
| 317 | ENDDO |
---|
| 318 | ENDDO |
---|
| 319 | |
---|
| 320 | ENDIF |
---|
| 321 | |
---|
| 322 | ! |
---|
| 323 | !-- Exchange boundaries for p |
---|
| 324 | CALL exchange_horiz( tend, 0, 0 ) |
---|
| 325 | |
---|
| 326 | ELSEIF ( psolver == 'sor' ) THEN |
---|
| 327 | |
---|
| 328 | ! |
---|
| 329 | !-- Solve Poisson equation for perturbation pressure using SOR-Red/Black |
---|
| 330 | !-- scheme |
---|
| 331 | CALL sor( d, ddzu, ddzw, p ) |
---|
| 332 | tend = p |
---|
| 333 | |
---|
| 334 | ELSEIF ( psolver == 'multigrid' ) THEN |
---|
| 335 | |
---|
| 336 | ! |
---|
| 337 | !-- Solve Poisson equation for perturbation pressure using Multigrid scheme, |
---|
| 338 | !-- array tend is used to store the residuals |
---|
| 339 | CALL poismg( tend ) |
---|
| 340 | |
---|
| 341 | ! |
---|
| 342 | !-- Restore perturbation pressure on tend because this array is used |
---|
| 343 | !-- further below to correct the velocity fields |
---|
| 344 | tend = p |
---|
| 345 | |
---|
| 346 | ENDIF |
---|
| 347 | |
---|
| 348 | ! |
---|
| 349 | !-- Store perturbation pressure on array p, used in the momentum equations |
---|
| 350 | IF ( psolver(1:7) == 'poisfft' ) THEN |
---|
| 351 | ! |
---|
| 352 | !-- Here, only the values from the left and right boundaries are copied |
---|
| 353 | !-- The remaining values are copied in the following loop due to speed |
---|
| 354 | !-- optimization |
---|
| 355 | !$OMP PARALLEL DO |
---|
| 356 | DO j = nys-1, nyn+1 |
---|
| 357 | DO k = nzb, nzt+1 |
---|
| 358 | p(k,j,nxl-1) = tend(k,j,nxl-1) |
---|
| 359 | p(k,j,nxr+1) = tend(k,j,nxr+1) |
---|
| 360 | ENDDO |
---|
| 361 | ENDDO |
---|
| 362 | ENDIF |
---|
| 363 | |
---|
| 364 | ! |
---|
| 365 | !-- Correction of the provisional velocities with the current perturbation |
---|
| 366 | !-- pressure just computed |
---|
| 367 | IF ( bc_lr /= 'cyclic' .OR. bc_ns /= 'cyclic' ) uvmean_outflow_l = 0.0 |
---|
| 368 | IF ( conserve_volume_flow ) THEN |
---|
| 369 | volume_flow_l(1) = 0.0 |
---|
| 370 | volume_flow_l(2) = 0.0 |
---|
| 371 | ENDIF |
---|
| 372 | !$OMP PARALLEL PRIVATE (i,j,k) |
---|
| 373 | !$OMP DO |
---|
| 374 | DO i = nxl, nxr |
---|
| 375 | IF ( psolver(1:7) == 'poisfft' ) THEN |
---|
| 376 | DO j = nys-1, nyn+1 |
---|
| 377 | DO k = nzb, nzt+1 |
---|
| 378 | p(k,j,i) = tend(k,j,i) |
---|
| 379 | ENDDO |
---|
| 380 | ENDDO |
---|
| 381 | ENDIF |
---|
| 382 | DO j = nys, nyn |
---|
| 383 | DO k = nzb_w_inner(j,i)+1, nzt |
---|
| 384 | w(k,j,i) = w(k,j,i) - dt_3d * & |
---|
| 385 | ( tend(k+1,j,i) - tend(k,j,i) ) * ddzu(k+1) |
---|
| 386 | ENDDO |
---|
| 387 | DO k = nzb_u_inner(j,i)+1, nzt |
---|
| 388 | u(k,j,i) = u(k,j,i) - dt_3d * ( tend(k,j,i) - tend(k,j,i-1) ) * ddx |
---|
| 389 | ENDDO |
---|
| 390 | DO k = nzb_v_inner(j,i)+1, nzt |
---|
| 391 | v(k,j,i) = v(k,j,i) - dt_3d * ( tend(k,j,i) - tend(k,j-1,i) ) * ddy |
---|
| 392 | ENDDO |
---|
| 393 | |
---|
| 394 | ! |
---|
| 395 | !-- Sum up the horizontal velocity along the outflow plane (in case |
---|
| 396 | !-- of non-cyclic boundary conditions). The respective mean velocity |
---|
| 397 | !-- is calculated from this in routine boundary_conds. |
---|
[73] | 398 | ! IF ( outflow_l .AND. i == nxl ) THEN |
---|
| 399 | ! !$OMP CRITICAL |
---|
| 400 | ! DO k = nzb, nzt+1 |
---|
| 401 | ! uvmean_outflow_l(k) = uvmean_outflow_l(k) + v(k,j,nxl) |
---|
| 402 | ! ENDDO |
---|
| 403 | ! !$OMP END CRITICAL |
---|
| 404 | ! ELSEIF ( outflow_r .AND. i == nxr ) THEN |
---|
| 405 | ! !$OMP CRITICAL |
---|
| 406 | ! DO k = nzb, nzt+1 |
---|
| 407 | ! uvmean_outflow_l(k) = uvmean_outflow_l(k) + v(k,j,nxr) |
---|
| 408 | ! ENDDO |
---|
| 409 | ! !$OMP END CRITICAL |
---|
| 410 | ! ELSEIF ( outflow_s .AND. j == nys ) THEN |
---|
| 411 | ! !$OMP CRITICAL |
---|
| 412 | ! DO k = nzb, nzt+1 |
---|
| 413 | ! uvmean_outflow_l(k) = uvmean_outflow_l(k) + u(k,nys,i) |
---|
| 414 | ! ENDDO |
---|
| 415 | ! !$OMP END CRITICAL |
---|
| 416 | ! ELSEIF ( outflow_n .AND. j == nyn ) THEN |
---|
| 417 | ! !$OMP CRITICAL |
---|
| 418 | ! DO k = nzb, nzt+1 |
---|
| 419 | ! uvmean_outflow_l(k) = uvmean_outflow_l(k) + u(k,nyn,i) |
---|
| 420 | ! ENDDO |
---|
| 421 | ! !$OMP END CRITICAL |
---|
| 422 | ! ENDIF |
---|
[1] | 423 | |
---|
| 424 | ! |
---|
| 425 | !-- Sum up the volume flow through the right and north boundary |
---|
| 426 | IF ( conserve_volume_flow .AND. i == nx ) THEN |
---|
| 427 | !$OMP CRITICAL |
---|
| 428 | DO k = nzb_2d(j,i) + 1, nzt |
---|
| 429 | volume_flow_l(1) = volume_flow_l(1) + u(k,j,i) * dzu(k) |
---|
| 430 | ENDDO |
---|
| 431 | !$OMP END CRITICAL |
---|
| 432 | ENDIF |
---|
| 433 | IF ( conserve_volume_flow .AND. j == ny ) THEN |
---|
| 434 | !$OMP CRITICAL |
---|
| 435 | DO k = nzb_2d(j,i) + 1, nzt |
---|
| 436 | volume_flow_l(2) = volume_flow_l(2) + v(k,j,i) * dzu(k) |
---|
| 437 | ENDDO |
---|
| 438 | !$OMP END CRITICAL |
---|
| 439 | ENDIF |
---|
| 440 | |
---|
| 441 | ENDDO |
---|
| 442 | ENDDO |
---|
| 443 | !$OMP END PARALLEL |
---|
| 444 | |
---|
| 445 | ! |
---|
| 446 | !-- Conserve the volume flow |
---|
| 447 | IF ( conserve_volume_flow ) THEN |
---|
| 448 | |
---|
| 449 | #if defined( __parallel ) |
---|
| 450 | CALL MPI_ALLREDUCE( volume_flow_l(1), volume_flow(1), 2, MPI_REAL, & |
---|
| 451 | MPI_SUM, comm2d, ierr ) |
---|
| 452 | #else |
---|
| 453 | volume_flow = volume_flow_l |
---|
| 454 | #endif |
---|
| 455 | |
---|
| 456 | volume_flow_offset = ( volume_flow_initial - volume_flow ) / & |
---|
| 457 | volume_flow_area |
---|
| 458 | |
---|
| 459 | !$OMP PARALLEL PRIVATE (i,j,k) |
---|
| 460 | !$OMP DO |
---|
| 461 | DO i = nxl, nxr |
---|
| 462 | DO j = nys, nyn |
---|
| 463 | DO k = nzb_u_inner(j,i) + 1, nzt |
---|
| 464 | u(k,j,i) = u(k,j,i) + volume_flow_offset(1) |
---|
| 465 | ENDDO |
---|
| 466 | DO k = nzb_v_inner(j,i) + 1, nzt |
---|
| 467 | v(k,j,i) = v(k,j,i) + volume_flow_offset(2) |
---|
| 468 | ENDDO |
---|
| 469 | ENDDO |
---|
| 470 | ENDDO |
---|
| 471 | !$OMP END PARALLEL |
---|
| 472 | |
---|
| 473 | ENDIF |
---|
| 474 | |
---|
| 475 | ! |
---|
| 476 | !-- Exchange of boundaries for the velocities |
---|
| 477 | CALL exchange_horiz( u, uxrp, 0 ) |
---|
| 478 | CALL exchange_horiz( v, 0, vynp ) |
---|
| 479 | CALL exchange_horiz( w, 0, 0 ) |
---|
| 480 | |
---|
| 481 | ! |
---|
| 482 | !-- Compute the divergence of the corrected velocity field, |
---|
| 483 | !-- a possible PE-sum is computed in flow_statistics |
---|
| 484 | CALL cpu_log( log_point_s(1), 'divergence', 'start' ) |
---|
| 485 | sums_divnew_l = 0.0 |
---|
| 486 | |
---|
| 487 | ! |
---|
| 488 | !-- d must be reset to zero because it can contain nonzero values below the |
---|
| 489 | !-- topography |
---|
| 490 | IF ( topography /= 'flat' ) d = 0.0 |
---|
| 491 | |
---|
| 492 | localsum = 0.0 |
---|
| 493 | threadsum = 0.0 |
---|
| 494 | |
---|
| 495 | !$OMP PARALLEL PRIVATE (i,j,k) FIRSTPRIVATE(threadsum) REDUCTION(+:localsum) |
---|
| 496 | !$OMP DO SCHEDULE( STATIC ) |
---|
| 497 | #if defined( __ibm ) |
---|
| 498 | DO i = nxl, nxr |
---|
| 499 | DO j = nys, nyn |
---|
| 500 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 501 | d(k,j,i) = ( u(k,j,i+1) - u(k,j,i) ) * ddx + & |
---|
| 502 | ( v(k,j+1,i) - v(k,j,i) ) * ddy + & |
---|
| 503 | ( w(k,j,i) - w(k-1,j,i) ) * ddzw(k) |
---|
| 504 | ENDDO |
---|
| 505 | DO k = nzb+1, nzt |
---|
| 506 | threadsum = threadsum + ABS( d(k,j,i) ) |
---|
| 507 | ENDDO |
---|
| 508 | ENDDO |
---|
| 509 | ENDDO |
---|
| 510 | #else |
---|
| 511 | DO i = nxl, nxr |
---|
| 512 | DO j = nys, nyn |
---|
| 513 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 514 | d(k,j,i) = ( u(k,j,i+1) - u(k,j,i) ) * ddx + & |
---|
| 515 | ( v(k,j+1,i) - v(k,j,i) ) * ddy + & |
---|
| 516 | ( w(k,j,i) - w(k-1,j,i) ) * ddzw(k) |
---|
| 517 | threadsum = threadsum + ABS( d(k,j,i) ) |
---|
| 518 | ENDDO |
---|
| 519 | ENDDO |
---|
| 520 | ENDDO |
---|
| 521 | #endif |
---|
| 522 | localsum = localsum + threadsum |
---|
| 523 | !$OMP END PARALLEL |
---|
| 524 | |
---|
| 525 | ! |
---|
| 526 | !-- For completeness, set the divergence sum of all statistic regions to those |
---|
| 527 | !-- of the total domain |
---|
| 528 | sums_divnew_l(0:statistic_regions) = localsum |
---|
| 529 | |
---|
| 530 | CALL cpu_log( log_point_s(1), 'divergence', 'stop' ) |
---|
| 531 | |
---|
| 532 | CALL cpu_log( log_point(8), 'pres', 'stop' ) |
---|
| 533 | |
---|
| 534 | |
---|
| 535 | END SUBROUTINE pres |
---|