| [1682] | 1 | !> @file lpm_droplet_condensation.f90 |
|---|
| [1036] | 2 | !--------------------------------------------------------------------------------! |
|---|
| 3 | ! This file is part of PALM. |
|---|
| 4 | ! |
|---|
| 5 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
|---|
| 6 | ! of the GNU General Public License as published by the Free Software Foundation, |
|---|
| 7 | ! either version 3 of the License, or (at your option) any later version. |
|---|
| 8 | ! |
|---|
| 9 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
|---|
| 10 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
|---|
| 11 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
|---|
| 12 | ! |
|---|
| 13 | ! You should have received a copy of the GNU General Public License along with |
|---|
| 14 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
|---|
| 15 | ! |
|---|
| [1818] | 16 | ! Copyright 1997-2016 Leibniz Universitaet Hannover |
|---|
| [1036] | 17 | !--------------------------------------------------------------------------------! |
|---|
| 18 | ! |
|---|
| [849] | 19 | ! Current revisions: |
|---|
| 20 | ! ------------------ |
|---|
| [1852] | 21 | ! |
|---|
| [1851] | 22 | ! |
|---|
| 23 | ! Former revisions: |
|---|
| 24 | ! ----------------- |
|---|
| 25 | ! $Id: lpm_droplet_condensation.f90 1852 2016-04-08 14:07:36Z maronga $ |
|---|
| 26 | ! |
|---|
| [1852] | 27 | ! |
|---|
| [1851] | 28 | ! 1849 2016-04-08 11:33:18Z hoffmann |
|---|
| [1852] | 29 | ! Interpolation of supersaturation has been removed because it is not in |
|---|
| 30 | ! accordance with the release/depletion of latent heat/water vapor in |
|---|
| [1849] | 31 | ! interaction_droplets_ptq. |
|---|
| 32 | ! Calculation of particle Reynolds number has been corrected. |
|---|
| [1852] | 33 | ! eps_ros added from modules. |
|---|
| [1849] | 34 | ! |
|---|
| [1832] | 35 | ! 1831 2016-04-07 13:15:51Z hoffmann |
|---|
| 36 | ! curvature_solution_effects moved to particle_attributes |
|---|
| 37 | ! |
|---|
| [1823] | 38 | ! 1822 2016-04-07 07:49:42Z hoffmann |
|---|
| 39 | ! Unused variables removed. |
|---|
| 40 | ! |
|---|
| [1683] | 41 | ! 1682 2015-10-07 23:56:08Z knoop |
|---|
| 42 | ! Code annotations made doxygen readable |
|---|
| 43 | ! |
|---|
| [1360] | 44 | ! 1359 2014-04-11 17:15:14Z hoffmann |
|---|
| 45 | ! New particle structure integrated. |
|---|
| 46 | ! Kind definition added to all floating point numbers. |
|---|
| 47 | ! |
|---|
| [1347] | 48 | ! 1346 2014-03-27 13:18:20Z heinze |
|---|
| 49 | ! Bugfix: REAL constants provided with KIND-attribute especially in call of |
|---|
| 50 | ! intrinsic function like MAX, MIN, SIGN |
|---|
| 51 | ! |
|---|
| [1323] | 52 | ! 1322 2014-03-20 16:38:49Z raasch |
|---|
| 53 | ! REAL constants defined as wp-kind |
|---|
| 54 | ! |
|---|
| [1321] | 55 | ! 1320 2014-03-20 08:40:49Z raasch |
|---|
| [1320] | 56 | ! ONLY-attribute added to USE-statements, |
|---|
| 57 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
|---|
| 58 | ! kinds are defined in new module kinds, |
|---|
| 59 | ! comment fields (!:) to be used for variable explanations added to |
|---|
| 60 | ! all variable declaration statements |
|---|
| [1072] | 61 | ! |
|---|
| [1319] | 62 | ! 1318 2014-03-17 13:35:16Z raasch |
|---|
| 63 | ! module interfaces removed |
|---|
| 64 | ! |
|---|
| [1093] | 65 | ! 1092 2013-02-02 11:24:22Z raasch |
|---|
| 66 | ! unused variables removed |
|---|
| 67 | ! |
|---|
| [1072] | 68 | ! 1071 2012-11-29 16:54:55Z franke |
|---|
| [1071] | 69 | ! Ventilation effect for evaporation of large droplets included |
|---|
| 70 | ! Check for unreasonable results included in calculation of Rosenbrock method |
|---|
| 71 | ! since physically unlikely results were observed and for the same |
|---|
| 72 | ! reason the first internal time step in Rosenbrock method should be < 1.0E02 in |
|---|
| 73 | ! case of evaporation |
|---|
| 74 | ! Unnecessary calculation of ql_int removed |
|---|
| 75 | ! Unnecessary calculations in Rosenbrock method (d2rdt2, drdt_m, dt_ros_last) |
|---|
| 76 | ! removed |
|---|
| 77 | ! Bugfix: factor in calculation of surface tension changed from 0.00155 to |
|---|
| 78 | ! 0.000155 |
|---|
| [849] | 79 | ! |
|---|
| [1037] | 80 | ! 1036 2012-10-22 13:43:42Z raasch |
|---|
| 81 | ! code put under GPL (PALM 3.9) |
|---|
| 82 | ! |
|---|
| [850] | 83 | ! 849 2012-03-15 10:35:09Z raasch |
|---|
| 84 | ! initial revision (former part of advec_particles) |
|---|
| [849] | 85 | ! |
|---|
| [850] | 86 | ! |
|---|
| [849] | 87 | ! Description: |
|---|
| 88 | ! ------------ |
|---|
| [1682] | 89 | !> Calculates change in droplet radius by condensation/evaporation, using |
|---|
| 90 | !> either an analytic formula or by numerically integrating the radius growth |
|---|
| 91 | !> equation including curvature and solution effects using Rosenbrocks method |
|---|
| 92 | !> (see Numerical recipes in FORTRAN, 2nd edition, p. 731). |
|---|
| 93 | !> The analytical formula and growth equation follow those given in |
|---|
| 94 | !> Rogers and Yau (A short course in cloud physics, 3rd edition, p. 102/103). |
|---|
| [849] | 95 | !------------------------------------------------------------------------------! |
|---|
| [1682] | 96 | SUBROUTINE lpm_droplet_condensation (ip,jp,kp) |
|---|
| 97 | |
|---|
| [849] | 98 | |
|---|
| [1320] | 99 | USE arrays_3d, & |
|---|
| [1849] | 100 | ONLY: hyp, pt, q, ql_c, ql_v |
|---|
| [849] | 101 | |
|---|
| [1320] | 102 | USE cloud_parameters, & |
|---|
| [1849] | 103 | ONLY: l_d_rv, l_v, rho_l, r_v |
|---|
| [849] | 104 | |
|---|
| [1320] | 105 | USE constants, & |
|---|
| 106 | ONLY: pi |
|---|
| [849] | 107 | |
|---|
| [1320] | 108 | USE control_parameters, & |
|---|
| [1822] | 109 | ONLY: dt_3d, dz, message_string, molecular_viscosity, rho_surface |
|---|
| 110 | |
|---|
| [1320] | 111 | USE cpulog, & |
|---|
| 112 | ONLY: cpu_log, log_point_s |
|---|
| [849] | 113 | |
|---|
| [1320] | 114 | USE grid_variables, & |
|---|
| [1822] | 115 | ONLY: dx, dy |
|---|
| [1071] | 116 | |
|---|
| [1320] | 117 | USE lpm_collision_kernels_mod, & |
|---|
| 118 | ONLY: rclass_lbound, rclass_ubound |
|---|
| [849] | 119 | |
|---|
| [1320] | 120 | USE kinds |
|---|
| 121 | |
|---|
| 122 | USE particle_attributes, & |
|---|
| [1849] | 123 | ONLY: curvature_solution_effects, hall_kernel, mass_of_solute, & |
|---|
| 124 | molecular_weight_of_solute, molecular_weight_of_water, & |
|---|
| 125 | number_of_particles, particles, radius_classes, & |
|---|
| 126 | use_kernel_tables, vanthoff, wang_kernel |
|---|
| [1320] | 127 | |
|---|
| 128 | |
|---|
| 129 | IMPLICIT NONE |
|---|
| 130 | |
|---|
| [1682] | 131 | INTEGER(iwp) :: i !< |
|---|
| 132 | INTEGER(iwp) :: ip !< |
|---|
| 133 | INTEGER(iwp) :: internal_timestep_count !< |
|---|
| 134 | INTEGER(iwp) :: j !< |
|---|
| 135 | INTEGER(iwp) :: jp !< |
|---|
| 136 | INTEGER(iwp) :: jtry !< |
|---|
| 137 | INTEGER(iwp) :: k !< |
|---|
| 138 | INTEGER(iwp) :: kp !< |
|---|
| 139 | INTEGER(iwp) :: n !< |
|---|
| 140 | INTEGER(iwp) :: ros_count !< |
|---|
| [1320] | 141 | |
|---|
| [1849] | 142 | INTEGER(iwp), PARAMETER :: maxtry = 40 !< |
|---|
| [1320] | 143 | |
|---|
| [1849] | 144 | LOGICAL :: repeat !< |
|---|
| [1320] | 145 | |
|---|
| [1682] | 146 | REAL(wp) :: aa !< |
|---|
| [1849] | 147 | REAL(wp) :: afactor !< curvature effects |
|---|
| [1682] | 148 | REAL(wp) :: arg !< |
|---|
| [1849] | 149 | REAL(wp) :: bfactor !< solute effects |
|---|
| [1682] | 150 | REAL(wp) :: ddenom !< |
|---|
| 151 | REAL(wp) :: delta_r !< |
|---|
| [1849] | 152 | REAL(wp) :: diameter !< diameter of cloud droplets |
|---|
| 153 | REAL(wp) :: diff_coeff_v !< diffusivity for water vapor |
|---|
| [1682] | 154 | REAL(wp) :: drdt !< |
|---|
| 155 | REAL(wp) :: drdt_ini !< |
|---|
| 156 | REAL(wp) :: dt_ros !< |
|---|
| 157 | REAL(wp) :: dt_ros_next !< |
|---|
| 158 | REAL(wp) :: dt_ros_sum !< |
|---|
| 159 | REAL(wp) :: dt_ros_sum_ini !< |
|---|
| 160 | REAL(wp) :: d2rdtdr !< |
|---|
| 161 | REAL(wp) :: errmax !< |
|---|
| [1849] | 162 | REAL(wp) :: e_a !< current vapor pressure |
|---|
| 163 | REAL(wp) :: e_s !< current saturation vapor pressure |
|---|
| [1682] | 164 | REAL(wp) :: err_ros !< |
|---|
| 165 | REAL(wp) :: g1 !< |
|---|
| 166 | REAL(wp) :: g2 !< |
|---|
| 167 | REAL(wp) :: g3 !< |
|---|
| 168 | REAL(wp) :: g4 !< |
|---|
| 169 | REAL(wp) :: r_ros !< |
|---|
| 170 | REAL(wp) :: r_ros_ini !< |
|---|
| 171 | REAL(wp) :: sigma !< |
|---|
| [1849] | 172 | REAL(wp) :: thermal_conductivity_v !< thermal conductivity for water |
|---|
| 173 | REAL(wp) :: t_int !< temperature |
|---|
| 174 | REAL(wp) :: w_s !< terminal velocity of droplets |
|---|
| [1682] | 175 | REAL(wp) :: re_p !< |
|---|
| [1849] | 176 | |
|---|
| 177 | ! |
|---|
| [849] | 178 | !-- Parameters for Rosenbrock method |
|---|
| [1682] | 179 | REAL(wp), PARAMETER :: a21 = 2.0_wp !< |
|---|
| 180 | REAL(wp), PARAMETER :: a31 = 48.0_wp / 25.0_wp !< |
|---|
| 181 | REAL(wp), PARAMETER :: a32 = 6.0_wp / 25.0_wp !< |
|---|
| 182 | REAL(wp), PARAMETER :: b1 = 19.0_wp / 9.0_wp !< |
|---|
| 183 | REAL(wp), PARAMETER :: b2 = 0.5_wp !< |
|---|
| 184 | REAL(wp), PARAMETER :: b3 = 25.0_wp / 108.0_wp !< |
|---|
| 185 | REAL(wp), PARAMETER :: b4 = 125.0_wp / 108.0_wp !< |
|---|
| 186 | REAL(wp), PARAMETER :: c21 = -8.0_wp !< |
|---|
| 187 | REAL(wp), PARAMETER :: c31 = 372.0_wp / 25.0_wp !< |
|---|
| 188 | REAL(wp), PARAMETER :: c32 = 12.0_wp / 5.0_wp !< |
|---|
| 189 | REAL(wp), PARAMETER :: c41 = -112.0_wp / 125.0_wp !< |
|---|
| 190 | REAL(wp), PARAMETER :: c42 = -54.0_wp / 125.0_wp !< |
|---|
| 191 | REAL(wp), PARAMETER :: c43 = -2.0_wp / 5.0_wp !< |
|---|
| 192 | REAL(wp), PARAMETER :: errcon = 0.1296_wp !< |
|---|
| 193 | REAL(wp), PARAMETER :: e1 = 17.0_wp / 54.0_wp !< |
|---|
| 194 | REAL(wp), PARAMETER :: e2 = 7.0_wp / 36.0_wp !< |
|---|
| 195 | REAL(wp), PARAMETER :: e3 = 0.0_wp !< |
|---|
| 196 | REAL(wp), PARAMETER :: e4 = 125.0_wp / 108.0_wp !< |
|---|
| 197 | REAL(wp), PARAMETER :: gam = 0.5_wp !< |
|---|
| 198 | REAL(wp), PARAMETER :: grow = 1.5_wp !< |
|---|
| 199 | REAL(wp), PARAMETER :: pgrow = -0.25_wp !< |
|---|
| 200 | REAL(wp), PARAMETER :: pshrnk = -1.0_wp /3.0_wp !< |
|---|
| 201 | REAL(wp), PARAMETER :: shrnk = 0.5_wp !< |
|---|
| [1849] | 202 | REAL(wp), PARAMETER :: eps_ros = 1.0E-4_wp !< accuracy of Rosenbrock method |
|---|
| [849] | 203 | |
|---|
| 204 | ! |
|---|
| [1849] | 205 | !-- Parameters for terminal velocity |
|---|
| 206 | REAL(wp), PARAMETER :: a_rog = 9.65_wp !< parameter for fall velocity |
|---|
| 207 | REAL(wp), PARAMETER :: b_rog = 10.43_wp !< parameter for fall velocity |
|---|
| 208 | REAL(wp), PARAMETER :: c_rog = 0.6_wp !< parameter for fall velocity |
|---|
| 209 | REAL(wp), PARAMETER :: k_cap_rog = 4.0_wp !< parameter for fall velocity |
|---|
| 210 | REAL(wp), PARAMETER :: k_low_rog = 12.0_wp !< parameter for fall velocity |
|---|
| 211 | REAL(wp), PARAMETER :: d0_rog = 0.745_wp !< separation diameter |
|---|
| [849] | 212 | |
|---|
| [1849] | 213 | REAL(wp), DIMENSION(number_of_particles) :: ventilation_effect !< |
|---|
| 214 | REAL(wp), DIMENSION(number_of_particles) :: new_r !< |
|---|
| [849] | 215 | |
|---|
| 216 | |
|---|
| 217 | |
|---|
| [1849] | 218 | CALL cpu_log( log_point_s(42), 'lpm_droplet_condens', 'start' ) |
|---|
| [849] | 219 | |
|---|
| 220 | ! |
|---|
| [1849] | 221 | !-- Calculate temperature, saturation vapor pressure and current vapor pressure |
|---|
| 222 | t_int = pt(kp,jp,ip) * ( hyp(kp) / 100000.0_wp )**0.286_wp |
|---|
| 223 | e_s = 611.0_wp * EXP( l_d_rv * ( 3.6609E-3_wp - 1.0_wp / t_int ) ) |
|---|
| 224 | e_a = q(kp,jp,ip) * hyp(kp) / ( 0.378_wp * q(kp,jp,ip) + 0.622_wp ) |
|---|
| [849] | 225 | ! |
|---|
| [1849] | 226 | !-- Thermal conductivity for water (from Rogers and Yau, Table 7.1), |
|---|
| 227 | !-- diffusivity for water vapor (after Hall und Pruppacher, 1976) |
|---|
| 228 | thermal_conductivity_v = 7.94048E-05_wp * t_int + 0.00227011_wp |
|---|
| 229 | diff_coeff_v = 0.211E-4_wp * ( t_int / 273.15_wp )**1.94_wp * & |
|---|
| 230 | ( 101325.0_wp / hyp(kp) ) |
|---|
| 231 | ! |
|---|
| 232 | !-- Calculate effects of heat conductivity and diffusion of water vapor on the |
|---|
| 233 | !-- condensation/evaporation process (typically known as 1.0 / (F_k + F_d) ) |
|---|
| 234 | ddenom = 1.0_wp / ( rho_l * r_v * t_int / ( e_s * diff_coeff_v ) + & |
|---|
| 235 | ( l_v / ( r_v * t_int ) - 1.0_wp ) * rho_l * & |
|---|
| 236 | l_v / ( thermal_conductivity_v * t_int ) & |
|---|
| 237 | ) |
|---|
| [849] | 238 | |
|---|
| [1359] | 239 | new_r = 0.0_wp |
|---|
| 240 | |
|---|
| [1849] | 241 | ! |
|---|
| 242 | !-- Determine ventilation effect on evaporation of large drops |
|---|
| [1359] | 243 | DO n = 1, number_of_particles |
|---|
| [1849] | 244 | |
|---|
| 245 | IF ( particles(n)%radius >= 4.0E-5_wp .AND. e_a / e_s < 1.0_wp ) THEN |
|---|
| [849] | 246 | ! |
|---|
| [1849] | 247 | !-- Terminal velocity is computed for vertical direction (Rogers et al., |
|---|
| 248 | !-- 1993, J. Appl. Meteorol.) |
|---|
| 249 | diameter = particles(n)%radius * 2000.0_wp !diameter in mm |
|---|
| 250 | IF ( diameter <= d0_rog ) THEN |
|---|
| 251 | w_s = k_cap_rog * diameter * ( 1.0_wp - EXP( -k_low_rog * diameter ) ) |
|---|
| 252 | ELSE |
|---|
| 253 | w_s = a_rog - b_rog * EXP( -c_rog * diameter ) |
|---|
| 254 | ENDIF |
|---|
| [849] | 255 | ! |
|---|
| [1849] | 256 | !-- First calculate droplet's Reynolds number |
|---|
| 257 | re_p = 2.0_wp * particles(n)%radius * w_s / molecular_viscosity |
|---|
| [1071] | 258 | ! |
|---|
| [1359] | 259 | !-- Ventilation coefficient (Rogers and Yau, 1989): |
|---|
| 260 | IF ( re_p > 2.5_wp ) THEN |
|---|
| [1849] | 261 | ventilation_effect(n) = 0.78_wp + 0.28_wp * SQRT( re_p ) |
|---|
| [1071] | 262 | ELSE |
|---|
| [1849] | 263 | ventilation_effect(n) = 1.0_wp + 0.09_wp * re_p |
|---|
| [1071] | 264 | ENDIF |
|---|
| [1849] | 265 | ELSE |
|---|
| [1071] | 266 | ! |
|---|
| [1849] | 267 | !-- For small droplets or in supersaturated environments, the ventilation |
|---|
| 268 | !-- effect does not play a role |
|---|
| 269 | ventilation_effect(n) = 1.0_wp |
|---|
| [849] | 270 | ENDIF |
|---|
| [1359] | 271 | ENDDO |
|---|
| [849] | 272 | |
|---|
| 273 | ! |
|---|
| [1849] | 274 | !-- Use analytic model for condensational growth |
|---|
| 275 | IF( .NOT. curvature_solution_effects ) then |
|---|
| 276 | DO n = 1, number_of_particles |
|---|
| 277 | arg = particles(n)%radius**2 + 2.0_wp * dt_3d * ddenom * & |
|---|
| 278 | ventilation_effect(n) * & |
|---|
| 279 | ( e_a / e_s - 1.0_wp ) |
|---|
| [1359] | 280 | arg = MAX( arg, 1.0E-16_wp ) |
|---|
| 281 | new_r(n) = SQRT( arg ) |
|---|
| [1849] | 282 | ENDDO |
|---|
| 283 | ENDIF |
|---|
| [1359] | 284 | |
|---|
| [1849] | 285 | ! |
|---|
| 286 | !-- If selected, use numerical solution of the condensational growth |
|---|
| 287 | !-- equation (e.g., for studying the activation of aerosols). |
|---|
| 288 | !-- Curvature and solutions effects are included in growth equation. |
|---|
| 289 | !-- Change in Radius is calculated with a 4th-order Rosenbrock method |
|---|
| 290 | !-- for stiff o.d.e's with monitoring local truncation error to adjust |
|---|
| 291 | !-- stepsize (see Numerical recipes in FORTRAN, 2nd edition, p. 731). |
|---|
| [1359] | 292 | DO n = 1, number_of_particles |
|---|
| [1849] | 293 | IF ( curvature_solution_effects ) THEN |
|---|
| [1071] | 294 | |
|---|
| 295 | ros_count = 0 |
|---|
| 296 | repeat = .TRUE. |
|---|
| [849] | 297 | ! |
|---|
| [1071] | 298 | !-- Carry out the Rosenbrock algorithm. In case of unreasonable results |
|---|
| 299 | !-- the switch "repeat" will be set true and the algorithm will be carried |
|---|
| 300 | !-- out again with the internal time step set to its initial (small) value. |
|---|
| [1359] | 301 | !-- Unreasonable results may occur if the external conditions, especially |
|---|
| 302 | !-- the supersaturation, has significantly changed compared to the last |
|---|
| 303 | !-- PALM timestep. |
|---|
| [1071] | 304 | DO WHILE ( repeat ) |
|---|
| [849] | 305 | |
|---|
| [1071] | 306 | repeat = .FALSE. |
|---|
| 307 | ! |
|---|
| [1849] | 308 | !-- Curvature effect (afactor) with surface tension parameterization |
|---|
| 309 | !-- by Straka (2009) |
|---|
| 310 | sigma = 0.0761_wp - 0.000155_wp * ( t_int - 273.15_wp ) |
|---|
| 311 | afactor = 2.0_wp * sigma / ( rho_l * r_v * t_int ) |
|---|
| 312 | ! |
|---|
| 313 | !-- Solute effect (bfactor), mass of solute to be replaced by variable |
|---|
| 314 | !-- aerosol radius |
|---|
| 315 | bfactor = 3.0_wp * vanthoff * mass_of_solute * & |
|---|
| 316 | molecular_weight_of_water / ( 4.0_wp * pi * rho_l * & |
|---|
| 317 | molecular_weight_of_solute & |
|---|
| 318 | ) |
|---|
| [849] | 319 | |
|---|
| [1071] | 320 | r_ros = particles(n)%radius |
|---|
| [1359] | 321 | dt_ros_sum = 0.0_wp ! internal integrated time (s) |
|---|
| [1071] | 322 | internal_timestep_count = 0 |
|---|
| [849] | 323 | ! |
|---|
| [1071] | 324 | !-- Take internal time step values from the end of last PALM time step |
|---|
| 325 | dt_ros_next = particles(n)%rvar1 |
|---|
| 326 | |
|---|
| [849] | 327 | ! |
|---|
| [1071] | 328 | !-- Internal time step should not be > 1.0E-2 in case of evaporation |
|---|
| 329 | !-- because larger values may lead to secondary solutions which are |
|---|
| 330 | !-- physically unlikely |
|---|
| [1849] | 331 | IF ( dt_ros_next > 1.0E-2_wp .AND. e_a / e_s < 1.0_wp ) THEN |
|---|
| [1359] | 332 | dt_ros_next = 1.0E-3_wp |
|---|
| [1071] | 333 | ENDIF |
|---|
| [849] | 334 | ! |
|---|
| [1071] | 335 | !-- If calculation of Rosenbrock method is repeated due to unreasonalble |
|---|
| 336 | !-- results during previous try the initial internal time step has to be |
|---|
| 337 | !-- reduced |
|---|
| 338 | IF ( ros_count > 1 ) THEN |
|---|
| [1359] | 339 | dt_ros_next = dt_ros_next - ( 0.2_wp * dt_ros_next ) |
|---|
| [1071] | 340 | ELSEIF ( ros_count > 5 ) THEN |
|---|
| [849] | 341 | ! |
|---|
| [1071] | 342 | !-- Prevent creation of infinite loop |
|---|
| 343 | message_string = 'ros_count > 5 in Rosenbrock method' |
|---|
| 344 | CALL message( 'lpm_droplet_condensation', 'PA0018', 2, 2, & |
|---|
| 345 | 0, 6, 0 ) |
|---|
| 346 | ENDIF |
|---|
| 347 | |
|---|
| [849] | 348 | ! |
|---|
| [1071] | 349 | !-- Internal time step must not be larger than PALM time step |
|---|
| 350 | dt_ros = MIN( dt_ros_next, dt_3d ) |
|---|
| 351 | ! |
|---|
| 352 | !-- Integrate growth equation in time unless PALM time step is reached |
|---|
| 353 | DO WHILE ( dt_ros_sum < dt_3d ) |
|---|
| [849] | 354 | |
|---|
| [1071] | 355 | internal_timestep_count = internal_timestep_count + 1 |
|---|
| [849] | 356 | |
|---|
| 357 | ! |
|---|
| [1071] | 358 | !-- Derivative at starting value |
|---|
| [1849] | 359 | drdt = ddenom * ventilation_effect(n) * ( e_a / e_s - 1.0_wp - & |
|---|
| 360 | afactor / r_ros + & |
|---|
| 361 | bfactor / r_ros**3 & |
|---|
| 362 | ) / r_ros |
|---|
| 363 | |
|---|
| [1071] | 364 | drdt_ini = drdt |
|---|
| 365 | dt_ros_sum_ini = dt_ros_sum |
|---|
| 366 | r_ros_ini = r_ros |
|---|
| [849] | 367 | |
|---|
| 368 | ! |
|---|
| [1071] | 369 | !-- Calculate radial derivative of dr/dt |
|---|
| [1849] | 370 | d2rdtdr = ddenom * ventilation_effect(n) * & |
|---|
| 371 | ( ( 1.0_wp - e_a / e_s ) / r_ros**2 + & |
|---|
| 372 | 2.0_wp * afactor / r_ros**3 - & |
|---|
| 373 | 4.0_wp * bfactor / r_ros**5 & |
|---|
| 374 | ) |
|---|
| [849] | 375 | ! |
|---|
| [1071] | 376 | !-- Adjust stepsize unless required accuracy is reached |
|---|
| 377 | DO jtry = 1, maxtry+1 |
|---|
| [849] | 378 | |
|---|
| [1071] | 379 | IF ( jtry == maxtry+1 ) THEN |
|---|
| 380 | message_string = 'maxtry > 40 in Rosenbrock method' |
|---|
| [1359] | 381 | CALL message( 'lpm_droplet_condensation', 'PA0347', 2, & |
|---|
| 382 | 2, 0, 6, 0 ) |
|---|
| [1071] | 383 | ENDIF |
|---|
| [849] | 384 | |
|---|
| [1359] | 385 | aa = 1.0_wp / ( gam * dt_ros ) - d2rdtdr |
|---|
| [1071] | 386 | g1 = drdt_ini / aa |
|---|
| 387 | r_ros = r_ros_ini + a21 * g1 |
|---|
| [1849] | 388 | drdt = ddenom * ventilation_effect(n) * ( e_a / e_s - 1.0_wp - & |
|---|
| 389 | afactor / r_ros + & |
|---|
| 390 | bfactor / r_ros**3 & |
|---|
| 391 | ) / r_ros |
|---|
| [849] | 392 | |
|---|
| [1071] | 393 | g2 = ( drdt + c21 * g1 / dt_ros )& |
|---|
| 394 | / aa |
|---|
| 395 | r_ros = r_ros_ini + a31 * g1 + a32 * g2 |
|---|
| [1849] | 396 | drdt = ddenom * ventilation_effect(n) * ( e_a / e_s - 1.0_wp - & |
|---|
| 397 | afactor / r_ros + & |
|---|
| 398 | bfactor / r_ros**3 & |
|---|
| 399 | ) / r_ros |
|---|
| [849] | 400 | |
|---|
| [1071] | 401 | g3 = ( drdt + & |
|---|
| 402 | ( c31 * g1 + c32 * g2 ) / dt_ros ) / aa |
|---|
| 403 | g4 = ( drdt + & |
|---|
| 404 | ( c41 * g1 + c42 * g2 + c43 * g3 ) / dt_ros ) / aa |
|---|
| 405 | r_ros = r_ros_ini + b1 * g1 + b2 * g2 + b3 * g3 + b4 * g4 |
|---|
| [849] | 406 | |
|---|
| [1071] | 407 | dt_ros_sum = dt_ros_sum_ini + dt_ros |
|---|
| [849] | 408 | |
|---|
| [1071] | 409 | IF ( dt_ros_sum == dt_ros_sum_ini ) THEN |
|---|
| 410 | message_string = 'zero stepsize in Rosenbrock method' |
|---|
| [1359] | 411 | CALL message( 'lpm_droplet_condensation', 'PA0348', 2, & |
|---|
| 412 | 2, 0, 6, 0 ) |
|---|
| [1071] | 413 | ENDIF |
|---|
| [849] | 414 | ! |
|---|
| [1071] | 415 | !-- Calculate error |
|---|
| [1359] | 416 | err_ros = e1 * g1 + e2 * g2 + e3 * g3 + e4 * g4 |
|---|
| 417 | errmax = 0.0_wp |
|---|
| [1071] | 418 | errmax = MAX( errmax, ABS( err_ros / r_ros_ini ) ) / eps_ros |
|---|
| [849] | 419 | ! |
|---|
| [1071] | 420 | !-- Leave loop if accuracy is sufficient, otherwise try again |
|---|
| 421 | !-- with a reduced stepsize |
|---|
| [1359] | 422 | IF ( errmax <= 1.0_wp ) THEN |
|---|
| [1071] | 423 | EXIT |
|---|
| 424 | ELSE |
|---|
| [1359] | 425 | dt_ros = SIGN( MAX( ABS( 0.9_wp * dt_ros * & |
|---|
| 426 | errmax**pshrnk ), & |
|---|
| 427 | shrnk * ABS( dt_ros ) ), dt_ros ) |
|---|
| [1071] | 428 | ENDIF |
|---|
| 429 | |
|---|
| 430 | ENDDO ! loop for stepsize adjustment |
|---|
| 431 | |
|---|
| 432 | ! |
|---|
| 433 | !-- Calculate next internal time step |
|---|
| 434 | IF ( errmax > errcon ) THEN |
|---|
| [1359] | 435 | dt_ros_next = 0.9_wp * dt_ros * errmax**pgrow |
|---|
| [849] | 436 | ELSE |
|---|
| [1071] | 437 | dt_ros_next = grow * dt_ros |
|---|
| [849] | 438 | ENDIF |
|---|
| 439 | |
|---|
| [1071] | 440 | ! |
|---|
| 441 | !-- Estimated time step is reduced if the PALM time step is exceeded |
|---|
| 442 | IF ( ( dt_ros_next + dt_ros_sum ) >= dt_3d ) THEN |
|---|
| 443 | dt_ros = dt_3d - dt_ros_sum |
|---|
| 444 | ELSE |
|---|
| 445 | dt_ros = dt_ros_next |
|---|
| 446 | ENDIF |
|---|
| [849] | 447 | |
|---|
| [1071] | 448 | ENDDO |
|---|
| [849] | 449 | ! |
|---|
| [1071] | 450 | !-- Store internal time step value for next PALM step |
|---|
| 451 | particles(n)%rvar1 = dt_ros_next |
|---|
| [849] | 452 | |
|---|
| [1359] | 453 | new_r(n) = r_ros |
|---|
| [849] | 454 | ! |
|---|
| [1071] | 455 | !-- Radius should not fall below 1E-8 because Rosenbrock method may |
|---|
| 456 | !-- lead to errors otherwise |
|---|
| [1359] | 457 | new_r(n) = MAX( new_r(n), 1.0E-8_wp ) |
|---|
| [1071] | 458 | ! |
|---|
| 459 | !-- Check if calculated droplet radius change is reasonable since in |
|---|
| 460 | !-- case of droplet evaporation the Rosenbrock method may lead to |
|---|
| 461 | !-- secondary solutions which are physically unlikely. |
|---|
| 462 | !-- Due to the solution effect the droplets may grow for relative |
|---|
| [1359] | 463 | !-- humidities below 100%, but change of radius should not be too |
|---|
| 464 | !-- large. In case of unreasonable droplet growth the Rosenbrock |
|---|
| 465 | !-- method is recalculated using a smaller initial time step. |
|---|
| [1071] | 466 | !-- Limiting values are tested for droplets down to 1.0E-7 |
|---|
| [1359] | 467 | IF ( new_r(n) - particles(n)%radius >= 3.0E-7_wp .AND. & |
|---|
| [1849] | 468 | e_a / e_s < 0.97_wp ) THEN |
|---|
| [1071] | 469 | ros_count = ros_count + 1 |
|---|
| 470 | repeat = .TRUE. |
|---|
| [849] | 471 | ENDIF |
|---|
| 472 | |
|---|
| [1071] | 473 | ENDDO ! Rosenbrock method |
|---|
| [849] | 474 | |
|---|
| 475 | ENDIF |
|---|
| 476 | |
|---|
| [1359] | 477 | delta_r = new_r(n) - particles(n)%radius |
|---|
| [849] | 478 | |
|---|
| 479 | ! |
|---|
| 480 | !-- Sum up the change in volume of liquid water for the respective grid |
|---|
| 481 | !-- volume (this is needed later in lpm_calc_liquid_water_content for |
|---|
| 482 | !-- calculating the release of latent heat) |
|---|
| [1359] | 483 | i = ip |
|---|
| 484 | j = jp |
|---|
| 485 | k = kp |
|---|
| [849] | 486 | ! only exact if equidistant |
|---|
| 487 | |
|---|
| [1359] | 488 | ql_c(k,j,i) = ql_c(k,j,i) + particles(n)%weight_factor * & |
|---|
| 489 | rho_l * 1.33333333_wp * pi * & |
|---|
| 490 | ( new_r(n)**3 - particles(n)%radius**3 ) / & |
|---|
| [849] | 491 | ( rho_surface * dx * dy * dz ) |
|---|
| [1359] | 492 | IF ( ql_c(k,j,i) > 100.0_wp ) THEN |
|---|
| [849] | 493 | WRITE( message_string, * ) 'k=',k,' j=',j,' i=',i, & |
|---|
| 494 | ' ql_c=',ql_c(k,j,i), ' &part(',n,')%wf=', & |
|---|
| 495 | particles(n)%weight_factor,' delta_r=',delta_r |
|---|
| 496 | CALL message( 'lpm_droplet_condensation', 'PA0143', 2, 2, -1, 6, 1 ) |
|---|
| 497 | ENDIF |
|---|
| 498 | |
|---|
| 499 | ! |
|---|
| 500 | !-- Change the droplet radius |
|---|
| [1359] | 501 | IF ( ( new_r(n) - particles(n)%radius ) < 0.0_wp .AND. & |
|---|
| 502 | new_r(n) < 0.0_wp ) THEN |
|---|
| 503 | WRITE( message_string, * ) '#1 k=',k,' j=',j,' i=',i, & |
|---|
| [1849] | 504 | ' e_s=',e_s, ' e_a=',e_a,' t_int=',t_int, & |
|---|
| [1359] | 505 | ' &delta_r=',delta_r, & |
|---|
| [849] | 506 | ' particle_radius=',particles(n)%radius |
|---|
| 507 | CALL message( 'lpm_droplet_condensation', 'PA0144', 2, 2, -1, 6, 1 ) |
|---|
| 508 | ENDIF |
|---|
| 509 | |
|---|
| 510 | ! |
|---|
| 511 | !-- Sum up the total volume of liquid water (needed below for |
|---|
| 512 | !-- re-calculating the weighting factors) |
|---|
| [1359] | 513 | ql_v(k,j,i) = ql_v(k,j,i) + particles(n)%weight_factor * new_r(n)**3 |
|---|
| [849] | 514 | |
|---|
| [1359] | 515 | particles(n)%radius = new_r(n) |
|---|
| [849] | 516 | |
|---|
| 517 | ! |
|---|
| 518 | !-- Determine radius class of the particle needed for collision |
|---|
| [1359] | 519 | IF ( ( hall_kernel .OR. wang_kernel ) .AND. use_kernel_tables ) & |
|---|
| [849] | 520 | THEN |
|---|
| [1359] | 521 | particles(n)%class = ( LOG( new_r(n) ) - rclass_lbound ) / & |
|---|
| 522 | ( rclass_ubound - rclass_lbound ) * & |
|---|
| [849] | 523 | radius_classes |
|---|
| 524 | particles(n)%class = MIN( particles(n)%class, radius_classes ) |
|---|
| 525 | particles(n)%class = MAX( particles(n)%class, 1 ) |
|---|
| 526 | ENDIF |
|---|
| 527 | |
|---|
| 528 | ENDDO |
|---|
| 529 | |
|---|
| 530 | CALL cpu_log( log_point_s(42), 'lpm_droplet_condens', 'stop' ) |
|---|
| 531 | |
|---|
| 532 | |
|---|
| 533 | END SUBROUTINE lpm_droplet_condensation |
|---|
