[1000] | 1 | MODULE microphysics_mod |
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| 2 | |
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[1093] | 3 | !--------------------------------------------------------------------------------! |
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| 4 | ! This file is part of PALM. |
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| 5 | ! |
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| 6 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
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| 7 | ! of the GNU General Public License as published by the Free Software Foundation, |
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| 8 | ! either version 3 of the License, or (at your option) any later version. |
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| 9 | ! |
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| 10 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
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| 11 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
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| 12 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
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| 13 | ! |
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| 14 | ! You should have received a copy of the GNU General Public License along with |
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| 15 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
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| 16 | ! |
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| 17 | ! Copyright 1997-2012 Leibniz University Hannover |
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| 18 | !--------------------------------------------------------------------------------! |
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| 19 | ! |
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[1000] | 20 | ! Current revisions: |
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[1092] | 21 | ! ------------------ |
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[1000] | 22 | ! |
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[1242] | 23 | ! |
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[1000] | 24 | ! Former revisions: |
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| 25 | ! ----------------- |
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[1052] | 26 | ! $Id: microphysics.f90 1242 2013-10-30 11:50:11Z fricke $ |
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[1054] | 27 | ! |
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[1242] | 28 | ! 1241 2013-10-30 11:36:58Z heinze |
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| 29 | ! hyp and rho have to be calculated at each time step if data from external |
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| 30 | ! file LSF_DATA are used |
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| 31 | ! |
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[1116] | 32 | ! 1115 2013-03-26 18:16:16Z hoffmann |
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| 33 | ! microphyical tendencies are calculated in microphysics_control in an optimized |
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| 34 | ! way; unrealistic values are prevented; bugfix in evaporation; some reformatting |
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| 35 | ! |
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[1107] | 36 | ! 1106 2013-03-04 05:31:38Z raasch |
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| 37 | ! small changes in code formatting |
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| 38 | ! |
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[1093] | 39 | ! 1092 2013-02-02 11:24:22Z raasch |
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| 40 | ! unused variables removed |
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| 41 | ! file put under GPL |
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| 42 | ! |
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[1066] | 43 | ! 1065 2012-11-22 17:42:36Z hoffmann |
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| 44 | ! Sedimentation process implemented according to Stevens and Seifert (2008). |
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[1115] | 45 | ! Turbulence effects on autoconversion and accretion added (Seifert, Nuijens |
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[1066] | 46 | ! and Stevens, 2010). |
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| 47 | ! |
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[1054] | 48 | ! 1053 2012-11-13 17:11:03Z hoffmann |
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| 49 | ! initial revision |
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[1000] | 50 | ! |
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| 51 | ! Description: |
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| 52 | ! ------------ |
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| 53 | ! Calculate cloud microphysics according to the two moment bulk |
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| 54 | ! scheme by Seifert and Beheng (2006). |
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| 55 | !------------------------------------------------------------------------------! |
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| 56 | |
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| 57 | PRIVATE |
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[1115] | 58 | PUBLIC microphysics_control |
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[1000] | 59 | |
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[1115] | 60 | INTERFACE microphysics_control |
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| 61 | MODULE PROCEDURE microphysics_control |
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| 62 | MODULE PROCEDURE microphysics_control_ij |
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| 63 | END INTERFACE microphysics_control |
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[1022] | 64 | |
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[1115] | 65 | INTERFACE adjust_cloud |
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| 66 | MODULE PROCEDURE adjust_cloud |
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| 67 | MODULE PROCEDURE adjust_cloud_ij |
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| 68 | END INTERFACE adjust_cloud |
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| 69 | |
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[1000] | 70 | INTERFACE autoconversion |
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| 71 | MODULE PROCEDURE autoconversion |
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| 72 | MODULE PROCEDURE autoconversion_ij |
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| 73 | END INTERFACE autoconversion |
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| 74 | |
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| 75 | INTERFACE accretion |
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| 76 | MODULE PROCEDURE accretion |
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| 77 | MODULE PROCEDURE accretion_ij |
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| 78 | END INTERFACE accretion |
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[1005] | 79 | |
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| 80 | INTERFACE selfcollection_breakup |
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| 81 | MODULE PROCEDURE selfcollection_breakup |
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| 82 | MODULE PROCEDURE selfcollection_breakup_ij |
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| 83 | END INTERFACE selfcollection_breakup |
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[1012] | 84 | |
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| 85 | INTERFACE evaporation_rain |
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| 86 | MODULE PROCEDURE evaporation_rain |
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| 87 | MODULE PROCEDURE evaporation_rain_ij |
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| 88 | END INTERFACE evaporation_rain |
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| 89 | |
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| 90 | INTERFACE sedimentation_cloud |
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| 91 | MODULE PROCEDURE sedimentation_cloud |
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| 92 | MODULE PROCEDURE sedimentation_cloud_ij |
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| 93 | END INTERFACE sedimentation_cloud |
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[1000] | 94 | |
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[1012] | 95 | INTERFACE sedimentation_rain |
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| 96 | MODULE PROCEDURE sedimentation_rain |
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| 97 | MODULE PROCEDURE sedimentation_rain_ij |
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| 98 | END INTERFACE sedimentation_rain |
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| 99 | |
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[1000] | 100 | CONTAINS |
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| 101 | |
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| 102 | |
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| 103 | !------------------------------------------------------------------------------! |
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| 104 | ! Call for all grid points |
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| 105 | !------------------------------------------------------------------------------! |
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[1115] | 106 | SUBROUTINE microphysics_control |
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[1022] | 107 | |
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| 108 | USE arrays_3d |
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[1241] | 109 | USE cloud_parameters |
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[1115] | 110 | USE control_parameters |
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[1241] | 111 | USE grid_variables |
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[1115] | 112 | USE indices |
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| 113 | USE statistics |
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| 114 | |
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| 115 | IMPLICIT NONE |
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| 116 | |
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| 117 | INTEGER :: i, j, k |
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| 118 | |
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| 119 | |
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| 120 | DO i = nxl, nxr |
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| 121 | DO j = nys, nyn |
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| 122 | DO k = nzb_s_inner(j,i)+1, nzt |
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| 123 | |
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| 124 | ENDDO |
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| 125 | ENDDO |
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| 126 | ENDDO |
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| 127 | |
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| 128 | END SUBROUTINE microphysics_control |
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| 129 | |
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| 130 | SUBROUTINE adjust_cloud |
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| 131 | |
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| 132 | USE arrays_3d |
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[1022] | 133 | USE cloud_parameters |
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| 134 | USE indices |
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| 135 | |
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| 136 | IMPLICIT NONE |
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| 137 | |
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| 138 | INTEGER :: i, j, k |
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| 139 | |
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| 140 | |
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| 141 | DO i = nxl, nxr |
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| 142 | DO j = nys, nyn |
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[1115] | 143 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1022] | 144 | |
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| 145 | ENDDO |
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| 146 | ENDDO |
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| 147 | ENDDO |
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| 148 | |
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[1115] | 149 | END SUBROUTINE adjust_cloud |
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[1022] | 150 | |
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[1106] | 151 | |
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[1000] | 152 | SUBROUTINE autoconversion |
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| 153 | |
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| 154 | USE arrays_3d |
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| 155 | USE cloud_parameters |
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[1115] | 156 | USE control_parameters |
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| 157 | USE grid_variables |
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[1000] | 158 | USE indices |
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| 159 | |
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| 160 | IMPLICIT NONE |
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| 161 | |
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| 162 | INTEGER :: i, j, k |
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| 163 | |
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| 164 | |
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| 165 | DO i = nxl, nxr |
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| 166 | DO j = nys, nyn |
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[1115] | 167 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1000] | 168 | |
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| 169 | ENDDO |
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| 170 | ENDDO |
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| 171 | ENDDO |
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| 172 | |
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| 173 | END SUBROUTINE autoconversion |
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| 174 | |
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[1106] | 175 | |
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[1005] | 176 | SUBROUTINE accretion |
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[1000] | 177 | |
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| 178 | USE arrays_3d |
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| 179 | USE cloud_parameters |
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[1115] | 180 | USE control_parameters |
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[1000] | 181 | USE indices |
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[1005] | 182 | |
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[1000] | 183 | IMPLICIT NONE |
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| 184 | |
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| 185 | INTEGER :: i, j, k |
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| 186 | |
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[1005] | 187 | |
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| 188 | DO i = nxl, nxr |
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| 189 | DO j = nys, nyn |
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[1115] | 190 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1000] | 191 | |
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[1005] | 192 | ENDDO |
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| 193 | ENDDO |
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[1000] | 194 | ENDDO |
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| 195 | |
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[1005] | 196 | END SUBROUTINE accretion |
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[1000] | 197 | |
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[1106] | 198 | |
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[1005] | 199 | SUBROUTINE selfcollection_breakup |
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[1000] | 200 | |
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| 201 | USE arrays_3d |
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| 202 | USE cloud_parameters |
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[1115] | 203 | USE control_parameters |
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[1000] | 204 | USE indices |
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| 205 | |
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| 206 | IMPLICIT NONE |
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| 207 | |
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| 208 | INTEGER :: i, j, k |
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| 209 | |
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| 210 | |
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| 211 | DO i = nxl, nxr |
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| 212 | DO j = nys, nyn |
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[1115] | 213 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1000] | 214 | |
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| 215 | ENDDO |
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| 216 | ENDDO |
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| 217 | ENDDO |
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| 218 | |
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[1005] | 219 | END SUBROUTINE selfcollection_breakup |
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[1000] | 220 | |
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[1106] | 221 | |
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[1012] | 222 | SUBROUTINE evaporation_rain |
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[1000] | 223 | |
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[1012] | 224 | USE arrays_3d |
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| 225 | USE cloud_parameters |
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| 226 | USE constants |
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[1115] | 227 | USE control_parameters |
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[1012] | 228 | USE indices |
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| 229 | |
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| 230 | IMPLICIT NONE |
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| 231 | |
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| 232 | INTEGER :: i, j, k |
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| 233 | |
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| 234 | |
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| 235 | DO i = nxl, nxr |
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| 236 | DO j = nys, nyn |
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[1115] | 237 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1012] | 238 | |
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| 239 | ENDDO |
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| 240 | ENDDO |
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| 241 | ENDDO |
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| 242 | |
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| 243 | END SUBROUTINE evaporation_rain |
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| 244 | |
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[1106] | 245 | |
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[1012] | 246 | SUBROUTINE sedimentation_cloud |
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| 247 | |
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| 248 | USE arrays_3d |
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| 249 | USE cloud_parameters |
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| 250 | USE constants |
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[1115] | 251 | USE control_parameters |
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[1012] | 252 | USE indices |
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| 253 | |
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| 254 | IMPLICIT NONE |
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| 255 | |
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| 256 | INTEGER :: i, j, k |
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| 257 | |
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| 258 | |
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| 259 | DO i = nxl, nxr |
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| 260 | DO j = nys, nyn |
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[1115] | 261 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1012] | 262 | |
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| 263 | ENDDO |
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| 264 | ENDDO |
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| 265 | ENDDO |
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| 266 | |
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| 267 | END SUBROUTINE sedimentation_cloud |
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| 268 | |
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[1106] | 269 | |
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[1012] | 270 | SUBROUTINE sedimentation_rain |
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| 271 | |
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| 272 | USE arrays_3d |
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| 273 | USE cloud_parameters |
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| 274 | USE constants |
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[1115] | 275 | USE control_parameters |
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[1012] | 276 | USE indices |
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[1115] | 277 | USE statistics |
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[1012] | 278 | |
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| 279 | IMPLICIT NONE |
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| 280 | |
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| 281 | INTEGER :: i, j, k |
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| 282 | |
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| 283 | |
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| 284 | DO i = nxl, nxr |
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| 285 | DO j = nys, nyn |
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[1115] | 286 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1012] | 287 | |
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| 288 | ENDDO |
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| 289 | ENDDO |
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| 290 | ENDDO |
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| 291 | |
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| 292 | END SUBROUTINE sedimentation_rain |
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| 293 | |
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| 294 | |
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[1000] | 295 | !------------------------------------------------------------------------------! |
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| 296 | ! Call for grid point i,j |
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| 297 | !------------------------------------------------------------------------------! |
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[1022] | 298 | |
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[1115] | 299 | SUBROUTINE microphysics_control_ij( i, j ) |
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| 300 | |
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[1022] | 301 | USE arrays_3d |
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| 302 | USE cloud_parameters |
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| 303 | USE control_parameters |
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[1241] | 304 | USE grid_variables |
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| 305 | USE indices |
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[1115] | 306 | USE statistics |
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| 307 | |
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[1022] | 308 | IMPLICIT NONE |
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| 309 | |
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[1241] | 310 | INTEGER :: i, j, k |
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| 311 | REAL :: t_surface |
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[1115] | 312 | |
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[1241] | 313 | IF ( large_scale_forcing .AND. lsf_surf ) THEN |
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| 314 | ! |
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| 315 | !-- Calculate: |
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| 316 | !-- pt / t : ratio of potential and actual temperature (pt_d_t) |
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| 317 | !-- t / pt : ratio of actual and potential temperature (t_d_pt) |
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| 318 | !-- p_0(z) : vertical profile of the hydrostatic pressure (hyp) |
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| 319 | t_surface = pt_surface * ( surface_pressure / 1000.0 )**0.286 |
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| 320 | DO k = nzb, nzt+1 |
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| 321 | hyp(k) = surface_pressure * 100.0 * & |
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| 322 | ( (t_surface - g/cp * zu(k)) / t_surface )**(1.0/0.286) |
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| 323 | pt_d_t(k) = ( 100000.0 / hyp(k) )**0.286 |
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| 324 | t_d_pt(k) = 1.0 / pt_d_t(k) |
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| 325 | hyrho(k) = hyp(k) / ( r_d * t_d_pt(k) * pt_init(k) ) |
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| 326 | ENDDO |
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| 327 | ! |
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| 328 | !-- Compute reference density |
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| 329 | rho_surface = surface_pressure * 100.0 / ( r_d * t_surface ) |
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| 330 | ENDIF |
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| 331 | |
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| 332 | |
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[1115] | 333 | dt_micro = dt_3d * weight_pres(intermediate_timestep_count) |
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| 334 | ! |
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| 335 | !-- Adjust unrealistic values |
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| 336 | IF ( precipitation ) CALL adjust_cloud( i,j ) |
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| 337 | ! |
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| 338 | !-- Use 1-d arrays |
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| 339 | q_1d(:) = q(:,j,i) |
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| 340 | pt_1d(:) = pt(:,j,i) |
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| 341 | qc_1d(:) = qc(:,j,i) |
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| 342 | nc_1d(:) = nc_const |
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| 343 | IF ( precipitation ) THEN |
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| 344 | qr_1d(:) = qr(:,j,i) |
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| 345 | nr_1d(:) = nr(:,j,i) |
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| 346 | ENDIF |
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| 347 | ! |
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| 348 | !-- Compute cloud physics |
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| 349 | IF ( precipitation ) THEN |
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| 350 | CALL autoconversion( i,j ) |
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| 351 | CALL accretion( i,j ) |
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| 352 | CALL selfcollection_breakup( i,j ) |
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| 353 | CALL evaporation_rain( i,j ) |
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| 354 | CALL sedimentation_rain( i,j ) |
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| 355 | ENDIF |
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| 356 | |
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| 357 | IF ( drizzle ) CALL sedimentation_cloud( i,j ) |
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| 358 | ! |
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| 359 | !-- Derive tendencies |
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| 360 | tend_q(:,j,i) = ( q_1d(:) - q(:,j,i) ) / dt_micro |
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| 361 | tend_pt(:,j,i) = ( pt_1d(:) - pt(:,j,i) ) / dt_micro |
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| 362 | IF ( precipitation ) THEN |
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| 363 | tend_qr(:,j,i) = ( qr_1d(:) - qr(:,j,i) ) / dt_micro |
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| 364 | tend_nr(:,j,i) = ( nr_1d(:) - nr(:,j,i) ) / dt_micro |
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| 365 | ENDIF |
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| 366 | |
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| 367 | END SUBROUTINE microphysics_control_ij |
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| 368 | |
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| 369 | SUBROUTINE adjust_cloud_ij( i, j ) |
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| 370 | |
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| 371 | USE arrays_3d |
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| 372 | USE cloud_parameters |
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| 373 | USE indices |
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| 374 | |
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| 375 | IMPLICIT NONE |
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| 376 | |
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[1022] | 377 | INTEGER :: i, j, k |
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[1115] | 378 | ! |
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| 379 | !-- Adjust number of raindrops to avoid nonlinear effects in |
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| 380 | !-- sedimentation and evaporation of rain drops due to too small or |
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| 381 | !-- too big weights of rain drops (Stevens and Seifert, 2008). |
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| 382 | !-- The same procedure is applied to cloud droplets if they are determined |
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| 383 | !-- prognostically. |
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| 384 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1022] | 385 | |
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[1065] | 386 | IF ( qr(k,j,i) <= eps_sb ) THEN |
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| 387 | qr(k,j,i) = 0.0 |
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[1115] | 388 | nr(k,j,i) = 0.0 |
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[1065] | 389 | ELSE |
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[1022] | 390 | ! |
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[1048] | 391 | !-- Adjust number of raindrops to avoid nonlinear effects in |
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| 392 | !-- sedimentation and evaporation of rain drops due to too small or |
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[1065] | 393 | !-- too big weights of rain drops (Stevens and Seifert, 2008). |
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| 394 | IF ( nr(k,j,i) * xrmin > qr(k,j,i) * hyrho(k) ) THEN |
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| 395 | nr(k,j,i) = qr(k,j,i) * hyrho(k) / xrmin |
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| 396 | ELSEIF ( nr(k,j,i) * xrmax < qr(k,j,i) * hyrho(k) ) THEN |
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| 397 | nr(k,j,i) = qr(k,j,i) * hyrho(k) / xrmax |
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[1048] | 398 | ENDIF |
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[1115] | 399 | |
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[1022] | 400 | ENDIF |
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[1115] | 401 | |
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[1022] | 402 | ENDDO |
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| 403 | |
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[1115] | 404 | END SUBROUTINE adjust_cloud_ij |
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[1022] | 405 | |
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[1106] | 406 | |
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[1005] | 407 | SUBROUTINE autoconversion_ij( i, j ) |
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[1000] | 408 | |
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| 409 | USE arrays_3d |
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| 410 | USE cloud_parameters |
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[1005] | 411 | USE control_parameters |
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[1065] | 412 | USE grid_variables |
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[1115] | 413 | USE indices |
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| 414 | |
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[1000] | 415 | IMPLICIT NONE |
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| 416 | |
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| 417 | INTEGER :: i, j, k |
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[1115] | 418 | REAL :: alpha_cc, autocon, epsilon, k_au, l_mix, nu_c, phi_au, & |
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| 419 | r_cc, rc, re_lambda, selfcoll, sigma_cc, tau_cloud, xc |
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[1000] | 420 | |
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[1106] | 421 | |
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[1005] | 422 | k_au = k_cc / ( 20.0 * x0 ) |
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| 423 | |
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[1115] | 424 | DO k = nzb_s_inner(j,i)+1, nzt |
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[1000] | 425 | |
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[1115] | 426 | IF ( qc_1d(k) > eps_sb ) THEN |
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[1012] | 427 | ! |
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[1048] | 428 | !-- Intern time scale of coagulation (Seifert and Beheng, 2006): |
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[1115] | 429 | !-- (1.0 - qc(k,j,i) / ( qc(k,j,i) + qr_1d(k) )) |
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| 430 | tau_cloud = 1.0 - qc_1d(k) / ( qr_1d(k) + qc_1d(k) ) |
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[1012] | 431 | ! |
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| 432 | !-- Universal function for autoconversion process |
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| 433 | !-- (Seifert and Beheng, 2006): |
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[1048] | 434 | phi_au = 600.0 * tau_cloud**0.68 * ( 1.0 - tau_cloud**0.68 )**3 |
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[1012] | 435 | ! |
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| 436 | !-- Shape parameter of gamma distribution (Geoffroy et al., 2010): |
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| 437 | !-- (Use constant nu_c = 1.0 instead?) |
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[1115] | 438 | nu_c = 1.0 !MAX( 0.0, 1580.0 * hyrho(k) * qc(k,j,i) - 0.28 ) |
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[1012] | 439 | ! |
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| 440 | !-- Mean weight of cloud droplets: |
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[1115] | 441 | xc = hyrho(k) * qc_1d(k) / nc_1d(k) |
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[1012] | 442 | ! |
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[1065] | 443 | !-- Parameterized turbulence effects on autoconversion (Seifert, |
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| 444 | !-- Nuijens and Stevens, 2010) |
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| 445 | IF ( turbulence ) THEN |
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| 446 | ! |
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| 447 | !-- Weight averaged radius of cloud droplets: |
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| 448 | rc = 0.5 * ( xc * dpirho_l )**( 1.0 / 3.0 ) |
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| 449 | |
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| 450 | alpha_cc = ( a_1 + a_2 * nu_c ) / ( 1.0 + a_3 * nu_c ) |
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| 451 | r_cc = ( b_1 + b_2 * nu_c ) / ( 1.0 + b_3 * nu_c ) |
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| 452 | sigma_cc = ( c_1 + c_2 * nu_c ) / ( 1.0 + c_3 * nu_c ) |
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| 453 | ! |
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| 454 | !-- Mixing length (neglecting distance to ground and stratification) |
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| 455 | l_mix = ( dx * dy * dzu(k) )**( 1.0 / 3.0 ) |
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| 456 | ! |
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| 457 | !-- Limit dissipation rate according to Seifert, Nuijens and |
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| 458 | !-- Stevens (2010) |
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| 459 | epsilon = MIN( 0.06, diss(k,j,i) ) |
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| 460 | ! |
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| 461 | !-- Compute Taylor-microscale Reynolds number: |
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| 462 | re_lambda = 6.0 / 11.0 * ( l_mix / c_const )**( 2.0 / 3.0 ) * & |
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| 463 | SQRT( 15.0 / kin_vis_air ) * epsilon**( 1.0 / 6.0 ) |
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| 464 | ! |
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| 465 | !-- The factor of 1.0E4 is needed to convert the dissipation rate |
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| 466 | !-- from m2 s-3 to cm2 s-3. |
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| 467 | k_au = k_au * ( 1.0 + & |
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| 468 | epsilon * 1.0E4 * ( re_lambda * 1.0E-3 )**0.25 * & |
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| 469 | ( alpha_cc * EXP( -1.0 * ( ( rc - r_cc ) / & |
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| 470 | sigma_cc )**2 ) + beta_cc ) ) |
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| 471 | ENDIF |
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| 472 | ! |
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[1012] | 473 | !-- Autoconversion rate (Seifert and Beheng, 2006): |
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[1115] | 474 | autocon = k_au * ( nu_c + 2.0 ) * ( nu_c + 4.0 ) / & |
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| 475 | ( nu_c + 1.0 )**2 * qc_1d(k)**2 * xc**2 * & |
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| 476 | ( 1.0 + phi_au / ( 1.0 - tau_cloud )**2 ) * & |
---|
| 477 | rho_surface |
---|
| 478 | autocon = MIN( autocon, qc_1d(k) / dt_micro ) |
---|
[1106] | 479 | |
---|
[1115] | 480 | qr_1d(k) = qr_1d(k) + autocon * dt_micro |
---|
| 481 | qc_1d(k) = qc_1d(k) - autocon * dt_micro |
---|
| 482 | nr_1d(k) = nr_1d(k) + autocon / x0 * hyrho(k) * dt_micro |
---|
| 483 | |
---|
[1005] | 484 | ENDIF |
---|
[1000] | 485 | |
---|
| 486 | ENDDO |
---|
| 487 | |
---|
[1005] | 488 | END SUBROUTINE autoconversion_ij |
---|
| 489 | |
---|
[1106] | 490 | |
---|
[1005] | 491 | SUBROUTINE accretion_ij( i, j ) |
---|
| 492 | |
---|
| 493 | USE arrays_3d |
---|
| 494 | USE cloud_parameters |
---|
[1115] | 495 | USE control_parameters |
---|
[1005] | 496 | USE indices |
---|
[1115] | 497 | |
---|
[1005] | 498 | IMPLICIT NONE |
---|
| 499 | |
---|
| 500 | INTEGER :: i, j, k |
---|
[1115] | 501 | REAL :: accr, k_cr, phi_ac, tau_cloud, xc |
---|
[1005] | 502 | |
---|
[1115] | 503 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 504 | IF ( ( qc_1d(k) > eps_sb ) .AND. ( qr_1d(k) > eps_sb ) ) THEN |
---|
[1012] | 505 | ! |
---|
[1048] | 506 | !-- Intern time scale of coagulation (Seifert and Beheng, 2006): |
---|
[1115] | 507 | tau_cloud = 1.0 - qc_1d(k) / ( qc_1d(k) + qr_1d(k) ) |
---|
[1012] | 508 | ! |
---|
| 509 | !-- Universal function for accretion process |
---|
[1048] | 510 | !-- (Seifert and Beheng, 2001): |
---|
[1065] | 511 | phi_ac = tau_cloud / ( tau_cloud + 5.0E-5 ) |
---|
| 512 | phi_ac = ( phi_ac**2 )**2 |
---|
[1012] | 513 | ! |
---|
[1065] | 514 | !-- Parameterized turbulence effects on autoconversion (Seifert, |
---|
| 515 | !-- Nuijens and Stevens, 2010). The factor of 1.0E4 is needed to |
---|
| 516 | !-- convert the dissipation (diss) from m2 s-3 to cm2 s-3. |
---|
| 517 | IF ( turbulence ) THEN |
---|
[1115] | 518 | k_cr = k_cr0 * ( 1.0 + 0.05 * & |
---|
[1065] | 519 | MIN( 600.0, diss(k,j,i) * 1.0E4 )**0.25 ) |
---|
| 520 | ELSE |
---|
| 521 | k_cr = k_cr0 |
---|
| 522 | ENDIF |
---|
| 523 | ! |
---|
[1012] | 524 | !-- Accretion rate (Seifert and Beheng, 2006): |
---|
[1115] | 525 | accr = k_cr * qc_1d(k) * qr_1d(k) * phi_ac * & |
---|
[1065] | 526 | SQRT( rho_surface * hyrho(k) ) |
---|
[1115] | 527 | accr = MIN( accr, qc_1d(k) / dt_micro ) |
---|
[1106] | 528 | |
---|
[1115] | 529 | qr_1d(k) = qr_1d(k) + accr * dt_micro |
---|
| 530 | qc_1d(k) = qc_1d(k) - accr * dt_micro |
---|
| 531 | |
---|
[1005] | 532 | ENDIF |
---|
[1106] | 533 | |
---|
[1005] | 534 | ENDDO |
---|
| 535 | |
---|
[1000] | 536 | END SUBROUTINE accretion_ij |
---|
| 537 | |
---|
[1005] | 538 | |
---|
| 539 | SUBROUTINE selfcollection_breakup_ij( i, j ) |
---|
| 540 | |
---|
| 541 | USE arrays_3d |
---|
| 542 | USE cloud_parameters |
---|
[1115] | 543 | USE control_parameters |
---|
[1005] | 544 | USE indices |
---|
| 545 | |
---|
| 546 | IMPLICIT NONE |
---|
| 547 | |
---|
| 548 | INTEGER :: i, j, k |
---|
[1115] | 549 | REAL :: breakup, dr, phi_br, selfcoll |
---|
[1005] | 550 | |
---|
[1115] | 551 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 552 | IF ( qr_1d(k) > eps_sb ) THEN |
---|
[1012] | 553 | ! |
---|
[1115] | 554 | !-- Selfcollection rate (Seifert and Beheng, 2001): |
---|
| 555 | selfcoll = k_rr * nr_1d(k) * qr_1d(k) * & |
---|
[1005] | 556 | SQRT( hyrho(k) * rho_surface ) |
---|
[1012] | 557 | ! |
---|
[1115] | 558 | !-- Weight averaged diameter of rain drops: |
---|
| 559 | dr = ( hyrho(k) * qr_1d(k) / nr_1d(k) * dpirho_l )**( 1.0 / 3.0 ) |
---|
| 560 | ! |
---|
[1048] | 561 | !-- Collisional breakup rate (Seifert, 2008): |
---|
[1115] | 562 | IF ( dr >= 0.3E-3 ) THEN |
---|
| 563 | phi_br = k_br * ( dr - 1.1E-3 ) |
---|
[1005] | 564 | breakup = selfcoll * ( phi_br + 1.0 ) |
---|
| 565 | ELSE |
---|
| 566 | breakup = 0.0 |
---|
| 567 | ENDIF |
---|
[1048] | 568 | |
---|
[1115] | 569 | selfcoll = MAX( breakup - selfcoll, -nr_1d(k) / dt_micro ) |
---|
| 570 | nr_1d(k) = nr_1d(k) + selfcoll * dt_micro |
---|
[1106] | 571 | |
---|
[1005] | 572 | ENDIF |
---|
| 573 | ENDDO |
---|
| 574 | |
---|
| 575 | END SUBROUTINE selfcollection_breakup_ij |
---|
| 576 | |
---|
[1106] | 577 | |
---|
[1012] | 578 | SUBROUTINE evaporation_rain_ij( i, j ) |
---|
[1022] | 579 | ! |
---|
| 580 | !-- Evaporation of precipitable water. Condensation is neglected for |
---|
| 581 | !-- precipitable water. |
---|
[1012] | 582 | |
---|
| 583 | USE arrays_3d |
---|
| 584 | USE cloud_parameters |
---|
| 585 | USE constants |
---|
[1115] | 586 | USE control_parameters |
---|
[1012] | 587 | USE indices |
---|
[1048] | 588 | |
---|
[1012] | 589 | IMPLICIT NONE |
---|
| 590 | |
---|
| 591 | INTEGER :: i, j, k |
---|
[1115] | 592 | REAL :: alpha, dr, e_s, evap, evap_nr, f_vent, g_evap, lambda_r, & |
---|
| 593 | mu_r, mu_r_2, mu_r_5d2, nr_0, q_s, sat, t_l, temp, xr |
---|
[1012] | 594 | |
---|
[1115] | 595 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 596 | IF ( qr_1d(k) > eps_sb ) THEN |
---|
[1012] | 597 | ! |
---|
| 598 | !-- Actual liquid water temperature: |
---|
[1115] | 599 | t_l = t_d_pt(k) * pt_1d(k) |
---|
[1012] | 600 | ! |
---|
| 601 | !-- Saturation vapor pressure at t_l: |
---|
| 602 | e_s = 610.78 * EXP( 17.269 * ( t_l - 273.16 ) / ( t_l - 35.86 ) ) |
---|
| 603 | ! |
---|
| 604 | !-- Computation of saturation humidity: |
---|
| 605 | q_s = 0.622 * e_s / ( hyp(k) - 0.378 * e_s ) |
---|
| 606 | alpha = 0.622 * l_d_r * l_d_cp / ( t_l * t_l ) |
---|
[1115] | 607 | q_s = q_s * ( 1.0 + alpha * q_1d(k) ) / ( 1.0 + alpha * q_s ) |
---|
[1012] | 608 | ! |
---|
[1106] | 609 | !-- Supersaturation: |
---|
[1115] | 610 | sat = MIN( 0.0, ( q_1d(k) - qr_1d(k) - qc_1d(k) ) / q_s - 1.0 ) |
---|
[1012] | 611 | ! |
---|
| 612 | !-- Actual temperature: |
---|
[1115] | 613 | temp = t_l + l_d_cp * ( qc_1d(k) + qr_1d(k) ) |
---|
| 614 | |
---|
| 615 | g_evap = 1.0 / ( ( l_v / ( r_v * temp ) - 1.0 ) * l_v / & |
---|
| 616 | ( thermal_conductivity_l * temp ) + r_v * temp / & |
---|
| 617 | ( diff_coeff_l * e_s ) ) |
---|
[1012] | 618 | ! |
---|
[1115] | 619 | !-- Mean weight of rain drops |
---|
| 620 | xr = hyrho(k) * qr_1d(k) / nr_1d(k) |
---|
[1012] | 621 | ! |
---|
[1115] | 622 | !-- Weight averaged diameter of rain drops: |
---|
| 623 | dr = ( xr * dpirho_l )**( 1.0 / 3.0 ) |
---|
| 624 | ! |
---|
[1049] | 625 | !-- Compute ventilation factor and intercept parameter |
---|
| 626 | !-- (Seifert and Beheng, 2006; Seifert, 2008): |
---|
[1048] | 627 | IF ( ventilation_effect ) THEN |
---|
[1115] | 628 | ! |
---|
| 629 | !-- Shape parameter of gamma distribution (Milbrandt and Yau, 2005; |
---|
| 630 | !-- Stevens and Seifert, 2008): |
---|
| 631 | mu_r = 10.0 * ( 1.0 + TANH( 1.2E3 * ( dr - 1.4E-3 ) ) ) |
---|
| 632 | ! |
---|
| 633 | !-- Slope parameter of gamma distribution (Seifert, 2008): |
---|
| 634 | lambda_r = ( ( mu_r + 3.0 ) * ( mu_r + 2.0 ) * & |
---|
| 635 | ( mu_r + 1.0 ) )**( 1.0 / 3.0 ) / dr |
---|
| 636 | |
---|
| 637 | mu_r_2 = mu_r + 2.0 |
---|
| 638 | mu_r_5d2 = mu_r + 2.5 |
---|
[1048] | 639 | f_vent = a_vent * gamm( mu_r_2 ) * & |
---|
[1115] | 640 | lambda_r**( -mu_r_2 ) + & |
---|
[1048] | 641 | b_vent * schmidt_p_1d3 * & |
---|
| 642 | SQRT( a_term / kin_vis_air ) * gamm( mu_r_5d2 ) * & |
---|
[1115] | 643 | lambda_r**( -mu_r_5d2 ) * & |
---|
[1048] | 644 | ( 1.0 - 0.5 * ( b_term / a_term ) * & |
---|
[1115] | 645 | ( lambda_r / & |
---|
| 646 | ( c_term + lambda_r ) )**mu_r_5d2 - & |
---|
[1048] | 647 | 0.125 * ( b_term / a_term )**2 * & |
---|
[1115] | 648 | ( lambda_r / & |
---|
| 649 | ( 2.0 * c_term + lambda_r ) )**mu_r_5d2 - & |
---|
[1048] | 650 | 0.0625 * ( b_term / a_term )**3 * & |
---|
[1115] | 651 | ( lambda_r / & |
---|
| 652 | ( 3.0 * c_term + lambda_r ) )**mu_r_5d2 - & |
---|
[1048] | 653 | 0.0390625 * ( b_term / a_term )**4 * & |
---|
[1115] | 654 | ( lambda_r / & |
---|
| 655 | ( 4.0 * c_term + lambda_r ) )**mu_r_5d2 ) |
---|
| 656 | nr_0 = nr_1d(k) * lambda_r**( mu_r + 1.0 ) / & |
---|
| 657 | gamm( mu_r + 1.0 ) |
---|
[1048] | 658 | ELSE |
---|
| 659 | f_vent = 1.0 |
---|
[1115] | 660 | nr_0 = nr_1d(k) * dr |
---|
[1048] | 661 | ENDIF |
---|
[1012] | 662 | ! |
---|
[1048] | 663 | !-- Evaporation rate of rain water content (Seifert and Beheng, 2006): |
---|
[1049] | 664 | evap = 2.0 * pi * nr_0 * g_evap * f_vent * sat / & |
---|
[1048] | 665 | hyrho(k) |
---|
[1106] | 666 | |
---|
[1115] | 667 | evap = MAX( evap, -qr_1d(k) / dt_micro ) |
---|
| 668 | evap_nr = MAX( c_evap * evap / xr * hyrho(k), & |
---|
| 669 | -nr_1d(k) / dt_micro ) |
---|
| 670 | |
---|
| 671 | qr_1d(k) = qr_1d(k) + evap * dt_micro |
---|
| 672 | nr_1d(k) = nr_1d(k) + evap_nr * dt_micro |
---|
[1012] | 673 | ENDIF |
---|
[1106] | 674 | |
---|
[1012] | 675 | ENDDO |
---|
| 676 | |
---|
| 677 | END SUBROUTINE evaporation_rain_ij |
---|
| 678 | |
---|
[1106] | 679 | |
---|
[1012] | 680 | SUBROUTINE sedimentation_cloud_ij( i, j ) |
---|
| 681 | |
---|
| 682 | USE arrays_3d |
---|
| 683 | USE cloud_parameters |
---|
| 684 | USE constants |
---|
[1115] | 685 | USE control_parameters |
---|
[1012] | 686 | USE indices |
---|
| 687 | |
---|
| 688 | IMPLICIT NONE |
---|
| 689 | |
---|
| 690 | INTEGER :: i, j, k |
---|
[1115] | 691 | REAL :: sed_qc_const |
---|
[1106] | 692 | |
---|
[1115] | 693 | REAL, DIMENSION(nzb:nzt+1) :: sed_qc |
---|
| 694 | |
---|
[1012] | 695 | ! |
---|
| 696 | !-- Sedimentation of cloud droplets (Heus et al., 2010): |
---|
[1115] | 697 | sed_qc_const = k_st * ( 3.0 / ( 4.0 * pi * rho_l ))**( 2.0 / 3.0 ) * & |
---|
[1048] | 698 | EXP( 5.0 * LOG( sigma_gc )**2 ) |
---|
[1012] | 699 | |
---|
[1115] | 700 | sed_qc(nzt+1) = 0.0 |
---|
[1012] | 701 | |
---|
[1115] | 702 | DO k = nzt, nzb_s_inner(j,i)+1, -1 |
---|
| 703 | IF ( qc_1d(k) > eps_sb ) THEN |
---|
| 704 | sed_qc(k) = sed_qc_const * nc_1d(k)**( -2.0 / 3.0 ) * & |
---|
| 705 | ( qc_1d(k) * hyrho(k) )**( 5.0 / 3.0 ) |
---|
| 706 | ELSE |
---|
| 707 | sed_qc(k) = 0.0 |
---|
[1012] | 708 | ENDIF |
---|
[1115] | 709 | |
---|
| 710 | sed_qc(k) = MIN( sed_qc(k), hyrho(k) * dzu(k+1) * q_1d(k) / & |
---|
| 711 | dt_micro + sed_qc(k+1) ) |
---|
| 712 | |
---|
| 713 | q_1d(k) = q_1d(k) + ( sed_qc(k+1) - sed_qc(k) ) * ddzu(k+1) / & |
---|
| 714 | hyrho(k) * dt_micro |
---|
| 715 | qc_1d(k) = qc_1d(k) + ( sed_qc(k+1) - sed_qc(k) ) * ddzu(k+1) / & |
---|
| 716 | hyrho(k) * dt_micro |
---|
| 717 | pt_1d(k) = pt_1d(k) - ( sed_qc(k+1) - sed_qc(k) ) * ddzu(k+1) / & |
---|
| 718 | hyrho(k) * l_d_cp * pt_d_t(k) * dt_micro |
---|
| 719 | |
---|
[1012] | 720 | ENDDO |
---|
| 721 | |
---|
| 722 | END SUBROUTINE sedimentation_cloud_ij |
---|
| 723 | |
---|
[1106] | 724 | |
---|
[1012] | 725 | SUBROUTINE sedimentation_rain_ij( i, j ) |
---|
| 726 | |
---|
| 727 | USE arrays_3d |
---|
| 728 | USE cloud_parameters |
---|
| 729 | USE constants |
---|
[1115] | 730 | USE control_parameters |
---|
[1012] | 731 | USE indices |
---|
[1048] | 732 | USE statistics |
---|
[1012] | 733 | |
---|
| 734 | IMPLICIT NONE |
---|
| 735 | |
---|
[1092] | 736 | INTEGER :: i, j, k, k_run |
---|
[1115] | 737 | REAL :: c_run, d_max, d_mean, d_min, dr, dt_sedi, flux, lambda_r, & |
---|
| 738 | mu_r, z_run |
---|
[1012] | 739 | |
---|
[1115] | 740 | REAL, DIMENSION(nzb:nzt+1) :: c_nr, c_qr, d_nr, d_qr, nr_slope, & |
---|
| 741 | qr_slope, sed_nr, sed_qr, w_nr, w_qr |
---|
[1065] | 742 | ! |
---|
| 743 | !-- Computation of sedimentation flux. Implementation according to Stevens |
---|
| 744 | !-- and Seifert (2008). |
---|
[1048] | 745 | IF ( intermediate_timestep_count == 1 ) prr(:,j,i) = 0.0 |
---|
[1012] | 746 | ! |
---|
[1065] | 747 | !-- Compute velocities |
---|
| 748 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
[1115] | 749 | IF ( qr_1d(k) > eps_sb ) THEN |
---|
| 750 | ! |
---|
| 751 | !-- Weight averaged diameter of rain drops: |
---|
| 752 | dr = ( hyrho(k) * qr_1d(k) / nr_1d(k) * dpirho_l )**( 1.0 / 3.0 ) |
---|
| 753 | ! |
---|
| 754 | !-- Shape parameter of gamma distribution (Milbrandt and Yau, 2005; |
---|
| 755 | !-- Stevens and Seifert, 2008): |
---|
| 756 | mu_r = 10.0 * ( 1.0 + TANH( 1.2E3 * ( dr - 1.4E-3 ) ) ) |
---|
| 757 | ! |
---|
| 758 | !-- Slope parameter of gamma distribution (Seifert, 2008): |
---|
| 759 | lambda_r = ( ( mu_r + 3.0 ) * ( mu_r + 2.0 ) * & |
---|
| 760 | ( mu_r + 1.0 ) )**( 1.0 / 3.0 ) / dr |
---|
| 761 | |
---|
[1065] | 762 | w_nr(k) = MAX( 0.1, MIN( 20.0, a_term - b_term * ( 1.0 + & |
---|
[1115] | 763 | c_term / lambda_r )**( -1.0 * ( mu_r + 1.0 ) ) ) ) |
---|
[1065] | 764 | w_qr(k) = MAX( 0.1, MIN( 20.0, a_term - b_term * ( 1.0 + & |
---|
[1115] | 765 | c_term / lambda_r )**( -1.0 * ( mu_r + 4.0 ) ) ) ) |
---|
[1065] | 766 | ELSE |
---|
| 767 | w_nr(k) = 0.0 |
---|
| 768 | w_qr(k) = 0.0 |
---|
| 769 | ENDIF |
---|
| 770 | ENDDO |
---|
[1048] | 771 | ! |
---|
[1065] | 772 | !-- Adjust boundary values |
---|
[1115] | 773 | w_nr(nzb_s_inner(j,i)) = w_nr(nzb_s_inner(j,i)+1) |
---|
| 774 | w_qr(nzb_s_inner(j,i)) = w_qr(nzb_s_inner(j,i)+1) |
---|
| 775 | w_nr(nzt+1) = 0.0 |
---|
| 776 | w_qr(nzt+1) = 0.0 |
---|
[1065] | 777 | ! |
---|
| 778 | !-- Compute Courant number |
---|
[1115] | 779 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
[1065] | 780 | c_nr(k) = 0.25 * ( w_nr(k-1) + 2.0 * w_nr(k) + w_nr(k+1) ) * & |
---|
[1115] | 781 | dt_micro * ddzu(k) |
---|
[1065] | 782 | c_qr(k) = 0.25 * ( w_qr(k-1) + 2.0 * w_qr(k) + w_qr(k+1) ) * & |
---|
[1115] | 783 | dt_micro * ddzu(k) |
---|
| 784 | ENDDO |
---|
[1065] | 785 | ! |
---|
| 786 | !-- Limit slopes with monotonized centered (MC) limiter (van Leer, 1977): |
---|
| 787 | IF ( limiter_sedimentation ) THEN |
---|
| 788 | |
---|
[1115] | 789 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
| 790 | d_mean = 0.5 * ( qr_1d(k+1) + qr_1d(k-1) ) |
---|
| 791 | d_min = qr_1d(k) - MIN( qr_1d(k+1), qr_1d(k), qr_1d(k-1) ) |
---|
| 792 | d_max = MAX( qr_1d(k+1), qr_1d(k), qr_1d(k-1) ) - qr_1d(k) |
---|
[1065] | 793 | |
---|
| 794 | qr_slope(k) = SIGN(1.0, d_mean) * MIN ( 2.0 * d_min, 2.0 * d_max, & |
---|
| 795 | ABS( d_mean ) ) |
---|
| 796 | |
---|
[1115] | 797 | d_mean = 0.5 * ( nr_1d(k+1) + nr_1d(k-1) ) |
---|
| 798 | d_min = nr_1d(k) - MIN( nr_1d(k+1), nr_1d(k), nr_1d(k-1) ) |
---|
| 799 | d_max = MAX( nr_1d(k+1), nr_1d(k), nr_1d(k-1) ) - nr_1d(k) |
---|
[1065] | 800 | |
---|
| 801 | nr_slope(k) = SIGN(1.0, d_mean) * MIN ( 2.0 * d_min, 2.0 * d_max, & |
---|
| 802 | ABS( d_mean ) ) |
---|
[1022] | 803 | ENDDO |
---|
[1048] | 804 | |
---|
[1065] | 805 | ELSE |
---|
[1106] | 806 | |
---|
[1065] | 807 | nr_slope = 0.0 |
---|
| 808 | qr_slope = 0.0 |
---|
[1106] | 809 | |
---|
[1065] | 810 | ENDIF |
---|
[1115] | 811 | |
---|
| 812 | sed_nr(nzt+1) = 0.0 |
---|
| 813 | sed_qr(nzt+1) = 0.0 |
---|
[1065] | 814 | ! |
---|
| 815 | !-- Compute sedimentation flux |
---|
[1115] | 816 | DO k = nzt, nzb_s_inner(j,i)+1, -1 |
---|
[1065] | 817 | ! |
---|
| 818 | !-- Sum up all rain drop number densities which contribute to the flux |
---|
| 819 | !-- through k-1/2 |
---|
| 820 | flux = 0.0 |
---|
| 821 | z_run = 0.0 ! height above z(k) |
---|
| 822 | k_run = k |
---|
| 823 | c_run = MIN( 1.0, c_nr(k) ) |
---|
[1115] | 824 | DO WHILE ( c_run > 0.0 .AND. k_run <= nzt ) |
---|
[1065] | 825 | flux = flux + hyrho(k_run) * & |
---|
[1115] | 826 | ( nr_1d(k_run) + nr_slope(k_run) * ( 1.0 - c_run ) * & |
---|
[1065] | 827 | 0.5 ) * c_run * dzu(k_run) |
---|
| 828 | z_run = z_run + dzu(k_run) |
---|
| 829 | k_run = k_run + 1 |
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| 830 | c_run = MIN( 1.0, c_nr(k_run) - z_run * ddzu(k_run) ) |
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[1022] | 831 | ENDDO |
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| 832 | ! |
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[1065] | 833 | !-- It is not allowed to sediment more rain drop number density than |
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| 834 | !-- available |
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| 835 | flux = MIN( flux, & |
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[1115] | 836 | hyrho(k) * dzu(k+1) * nr_1d(k) + sed_nr(k+1) * dt_micro ) |
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[1065] | 837 | |
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[1115] | 838 | sed_nr(k) = flux / dt_micro |
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| 839 | nr_1d(k) = nr_1d(k) + ( sed_nr(k+1) - sed_nr(k) ) * ddzu(k+1) / & |
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| 840 | hyrho(k) * dt_micro |
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[1065] | 841 | ! |
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| 842 | !-- Sum up all rain water content which contributes to the flux |
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| 843 | !-- through k-1/2 |
---|
| 844 | flux = 0.0 |
---|
| 845 | z_run = 0.0 ! height above z(k) |
---|
| 846 | k_run = k |
---|
| 847 | c_run = MIN( 1.0, c_qr(k) ) |
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[1106] | 848 | |
---|
[1065] | 849 | DO WHILE ( c_run > 0.0 .AND. k_run <= nzt-1 ) |
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[1106] | 850 | |
---|
[1065] | 851 | flux = flux + hyrho(k_run) * & |
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[1115] | 852 | ( qr_1d(k_run) + qr_slope(k_run) * ( 1.0 - c_run ) * & |
---|
[1065] | 853 | 0.5 ) * c_run * dzu(k_run) |
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| 854 | z_run = z_run + dzu(k_run) |
---|
| 855 | k_run = k_run + 1 |
---|
| 856 | c_run = MIN( 1.0, c_qr(k_run) - z_run * ddzu(k_run) ) |
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[1106] | 857 | |
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[1065] | 858 | ENDDO |
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| 859 | ! |
---|
| 860 | !-- It is not allowed to sediment more rain water content than available |
---|
| 861 | flux = MIN( flux, & |
---|
[1115] | 862 | hyrho(k) * dzu(k) * qr_1d(k) + sed_qr(k+1) * dt_micro ) |
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[1065] | 863 | |
---|
[1115] | 864 | sed_qr(k) = flux / dt_micro |
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| 865 | |
---|
| 866 | qr_1d(k) = qr_1d(k) + ( sed_qr(k+1) - sed_qr(k) ) * ddzu(k+1) / & |
---|
| 867 | hyrho(k) * dt_micro |
---|
| 868 | q_1d(k) = q_1d(k) + ( sed_qr(k+1) - sed_qr(k) ) * ddzu(k+1) / & |
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| 869 | hyrho(k) * dt_micro |
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| 870 | pt_1d(k) = pt_1d(k) - ( sed_qr(k+1) - sed_qr(k) ) * ddzu(k+1) / & |
---|
| 871 | hyrho(k) * l_d_cp * pt_d_t(k) * dt_micro |
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[1065] | 872 | ! |
---|
| 873 | !-- Compute the rain rate |
---|
| 874 | prr(k,j,i) = prr(k,j,i) + sed_qr(k) / hyrho(k) * & |
---|
[1115] | 875 | weight_substep(intermediate_timestep_count) |
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[1065] | 876 | ENDDO |
---|
[1115] | 877 | |
---|
[1065] | 878 | ! |
---|
[1048] | 879 | !-- Precipitation amount |
---|
| 880 | IF ( intermediate_timestep_count == intermediate_timestep_count_max & |
---|
| 881 | .AND. ( dt_do2d_xy - time_do2d_xy ) < & |
---|
| 882 | precipitation_amount_interval ) THEN |
---|
[1012] | 883 | |
---|
[1048] | 884 | precipitation_amount(j,i) = precipitation_amount(j,i) + & |
---|
[1115] | 885 | prr(nzb_s_inner(j,i)+1,j,i) * & |
---|
| 886 | hyrho(nzb_s_inner(j,i)+1) * dt_3d |
---|
[1048] | 887 | ENDIF |
---|
| 888 | |
---|
[1012] | 889 | END SUBROUTINE sedimentation_rain_ij |
---|
| 890 | |
---|
[1106] | 891 | |
---|
[1012] | 892 | ! |
---|
| 893 | !-- This function computes the gamma function (Press et al., 1992). |
---|
| 894 | !-- The gamma function is needed for the calculation of the evaporation |
---|
| 895 | !-- of rain drops. |
---|
| 896 | FUNCTION gamm( xx ) |
---|
[1048] | 897 | |
---|
| 898 | USE cloud_parameters |
---|
[1012] | 899 | |
---|
| 900 | IMPLICIT NONE |
---|
| 901 | |
---|
[1065] | 902 | REAL :: gamm, ser, tmp, x_gamm, xx, y_gamm |
---|
[1012] | 903 | INTEGER :: j |
---|
[1106] | 904 | |
---|
[1012] | 905 | |
---|
| 906 | x_gamm = xx |
---|
| 907 | y_gamm = x_gamm |
---|
| 908 | tmp = x_gamm + 5.5 |
---|
| 909 | tmp = ( x_gamm + 0.5 ) * LOG( tmp ) - tmp |
---|
| 910 | ser = 1.000000000190015 |
---|
[1106] | 911 | |
---|
| 912 | DO j = 1, 6 |
---|
[1012] | 913 | y_gamm = y_gamm + 1.0 |
---|
| 914 | ser = ser + cof( j ) / y_gamm |
---|
[1106] | 915 | ENDDO |
---|
| 916 | |
---|
[1012] | 917 | ! |
---|
| 918 | !-- Until this point the algorithm computes the logarithm of the gamma |
---|
| 919 | !-- function. Hence, the exponential function is used. |
---|
| 920 | ! gamm = EXP( tmp + LOG( stp * ser / x_gamm ) ) |
---|
| 921 | gamm = EXP( tmp ) * stp * ser / x_gamm |
---|
[1106] | 922 | |
---|
[1012] | 923 | RETURN |
---|
| 924 | |
---|
| 925 | END FUNCTION gamm |
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| 926 | |
---|
| 927 | END MODULE microphysics_mod |
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