1 | !********************************************************************** |
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2 | ! Copyright 1998,1999,2000,2001,2002,2005,2007,2008,2009,2010 * |
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3 | ! Andreas Stohl, Petra Seibert, A. Frank, Gerhard Wotawa, * |
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4 | ! Caroline Forster, Sabine Eckhardt, John Burkhart, Harald Sodemann * |
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5 | ! * |
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6 | ! This file is part of FLEXPART. * |
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7 | ! * |
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8 | ! FLEXPART is free software: you can redistribute it and/or modify * |
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9 | ! it under the terms of the GNU General Public License as published by* |
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10 | ! the Free Software Foundation, either version 3 of the License, or * |
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11 | ! (at your option) any later version. * |
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12 | ! * |
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13 | ! FLEXPART is distributed in the hope that it will be useful, * |
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14 | ! but WITHOUT ANY WARRANTY; without even the implied warranty of * |
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15 | ! MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the * |
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16 | ! GNU General Public License for more details. * |
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17 | ! * |
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18 | ! You should have received a copy of the GNU General Public License * |
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19 | ! along with FLEXPART. If not, see <http://www.gnu.org/licenses/>. * |
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20 | !********************************************************************** |
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21 | |
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22 | subroutine boundcond_domainfill(itime,loutend) |
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23 | ! i i |
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24 | !***************************************************************************** |
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25 | ! * |
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26 | ! Particles are created by this subroutine continuously throughout the * |
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27 | ! simulation at the boundaries of the domain-filling box. * |
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28 | ! All particles carry the same amount of mass which alltogether comprises the* |
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29 | ! mass of air within the box, which remains (more or less) constant. * |
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30 | ! * |
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31 | ! Author: A. Stohl * |
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32 | ! * |
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33 | ! 16 October 2002 * |
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34 | ! * |
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35 | !***************************************************************************** |
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36 | ! * |
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37 | ! Variables: * |
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38 | ! * |
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39 | ! nx_we(2) grid indices for western and eastern boundary of domain- * |
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40 | ! filling trajectory calculations * |
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41 | ! ny_sn(2) grid indices for southern and northern boundary of domain- * |
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42 | ! filling trajectory calculations * |
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43 | ! * |
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44 | !***************************************************************************** |
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45 | ! CHANGES |
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46 | ! 08/2016 eso: MPI version: |
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47 | ! |
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48 | ! -Root process release particles and distributes to other processes. |
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49 | ! Temporary arrays are used, also for the non-root (receiving) processes. |
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50 | ! -The scheme can be improved by having all processes report numpart |
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51 | ! (keeping track of how many particles have left the domain), so that |
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52 | ! a proportional amount of new particles can be distributed (however |
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53 | ! we have a separate function called from timemanager that will |
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54 | ! redistribute particles among processes if there are imbalances) |
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55 | !***************************************************************************** |
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56 | |
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57 | use point_mod |
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58 | use par_mod |
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59 | use com_mod |
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60 | use random_mod, only: ran1 |
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61 | use mpi_mod |
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62 | |
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63 | implicit none |
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64 | |
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65 | real :: dz,dz1,dz2,dt1,dt2,dtt,ylat,xm,cosfact,accmasst |
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66 | integer :: itime,in,indz,indzp,i,loutend |
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67 | integer :: j,k,ix,jy,m,indzh,indexh,minpart,ipart,mmass |
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68 | integer :: numactiveparticles, numpart_total, rel_counter |
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69 | integer,allocatable,dimension(:) :: numrel_mpi !, numactiveparticles_mpi |
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70 | |
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71 | real :: windl(2),rhol(2) |
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72 | real :: windhl(2),rhohl(2) |
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73 | real :: windx,rhox |
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74 | real :: deltaz,boundarea,fluxofmass |
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75 | |
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76 | integer :: ixm,ixp,jym,jyp,indzm,mm |
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77 | real :: pvpart,ddx,ddy,rddx,rddy,p1,p2,p3,p4,y1(2),yh1(2) |
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78 | |
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79 | integer :: idummy = -11 |
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80 | integer :: mtag |
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81 | logical :: first_call=.true. |
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82 | ! Sizes of temporary arrays are maxpartfract*maxpart. Increase maxpartfract if |
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83 | ! needed. |
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84 | real,parameter :: maxpartfract=0.1 |
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85 | integer :: tmp_size = int(maxpartfract*maxpart) |
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86 | |
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87 | ! Use different seed for each process |
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88 | if (first_call) then |
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89 | idummy=idummy+mp_seed |
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90 | first_call=.false. |
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91 | end if |
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92 | |
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93 | |
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94 | ! If domain-filling is global, no boundary conditions are needed |
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95 | !*************************************************************** |
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96 | |
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97 | if (gdomainfill) return |
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98 | |
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99 | accmasst=0. |
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100 | numactiveparticles=0 |
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101 | ! Keep track of active particles on each process |
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102 | allocate(numrel_mpi(0:mp_partgroup_np-1)) |
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103 | ! numactiveparticles_mpi(0:mp_partgroup_np-1) |
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104 | |
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105 | ! New particles to be released on each process |
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106 | numrel_mpi(:)=0 |
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107 | |
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108 | ! Terminate trajectories that have left the domain, if domain-filling |
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109 | ! trajectory calculation domain is not global. Done for all processes |
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110 | !******************************************************************** |
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111 | |
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112 | do i=1,numpart |
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113 | if (itra1(i).eq.itime) then |
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114 | if ((ytra1(i).gt.real(ny_sn(2))).or. & |
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115 | (ytra1(i).lt.real(ny_sn(1)))) itra1(i)=-999999999 |
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116 | if (((.not.xglobal).or.(nx_we(2).ne.(nx-2))).and. & |
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117 | ((xtra1(i).lt.real(nx_we(1))).or. & |
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118 | (xtra1(i).gt.real(nx_we(2))))) itra1(i)=-999999999 |
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119 | endif |
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120 | if (itra1(i).ne.-999999999) numactiveparticles= & |
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121 | numactiveparticles+1 |
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122 | end do |
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123 | ! numactiveparticles_mpi(mp_partid) = numactiveparticles |
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124 | |
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125 | |
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126 | ! Collect number of active particles from all processes |
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127 | ! call MPI_Allgather(numactiveparticles, 1, MPI_INTEGER, & |
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128 | ! &numactiveparticles_mpi, 1, MPI_INTEGER, mp_comm_used, mp_ierr) |
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129 | |
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130 | |
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131 | ! Total number of new releases |
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132 | numpart_total = 0 |
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133 | |
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134 | |
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135 | ! This section only done by root process |
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136 | !*************************************** |
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137 | |
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138 | if (lroot) then |
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139 | |
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140 | ! Use separate arrays for newly released particles |
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141 | !************************************************* |
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142 | |
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143 | allocate(itra1_tmp(tmp_size),npoint_tmp(tmp_size),nclass_tmp(tmp_size),& |
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144 | & idt_tmp(tmp_size),itramem_tmp(tmp_size),itrasplit_tmp(tmp_size),& |
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145 | & xtra1_tmp(tmp_size),ytra1_tmp(tmp_size),ztra1_tmp(tmp_size),& |
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146 | & xmass1_tmp(tmp_size, maxspec)) |
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147 | |
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148 | ! Initialize all particles as non-existent |
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149 | itra1_tmp(:)=-999999999 |
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150 | |
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151 | ! Determine auxiliary variables for time interpolation |
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152 | !***************************************************** |
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153 | |
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154 | dt1=real(itime-memtime(1)) |
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155 | dt2=real(memtime(2)-itime) |
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156 | dtt=1./(dt1+dt2) |
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157 | |
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158 | ! Initialize auxiliary variable used to search for vacant storage space |
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159 | !********************************************************************** |
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160 | |
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161 | minpart=1 |
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162 | |
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163 | !*************************************** |
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164 | ! Western and eastern boundary condition |
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165 | !*************************************** |
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166 | |
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167 | ! Loop from south to north |
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168 | !************************* |
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169 | |
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170 | do jy=ny_sn(1),ny_sn(2) |
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171 | |
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172 | ! Loop over western (index 1) and eastern (index 2) boundary |
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173 | !*********************************************************** |
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174 | |
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175 | do k=1,2 |
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176 | |
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177 | ! Loop over all release locations in a column |
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178 | !******************************************** |
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179 | |
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180 | do j=1,numcolumn_we(k,jy) |
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181 | |
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182 | ! Determine, for each release location, the area of the corresponding boundary |
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183 | !***************************************************************************** |
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184 | |
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185 | if (j.eq.1) then |
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186 | deltaz=(zcolumn_we(k,jy,2)+zcolumn_we(k,jy,1))/2. |
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187 | else if (j.eq.numcolumn_we(k,jy)) then |
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188 | ! deltaz=height(nz)-(zcolumn_we(k,jy,j-1)+ |
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189 | ! + zcolumn_we(k,jy,j))/2. |
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190 | ! In order to avoid taking a very high column for very many particles, |
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191 | ! use the deltaz from one particle below instead |
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192 | deltaz=(zcolumn_we(k,jy,j)-zcolumn_we(k,jy,j-2))/2. |
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193 | else |
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194 | deltaz=(zcolumn_we(k,jy,j+1)-zcolumn_we(k,jy,j-1))/2. |
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195 | endif |
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196 | if ((jy.eq.ny_sn(1)).or.(jy.eq.ny_sn(2))) then |
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197 | boundarea=deltaz*111198.5/2.*dy |
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198 | else |
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199 | boundarea=deltaz*111198.5*dy |
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200 | endif |
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201 | |
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202 | |
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203 | ! Interpolate the wind velocity and density to the release location |
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204 | !****************************************************************** |
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205 | |
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206 | ! Determine the model level below the release position |
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207 | !***************************************************** |
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208 | |
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209 | do i=2,nz |
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210 | if (height(i).gt.zcolumn_we(k,jy,j)) then |
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211 | indz=i-1 |
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212 | indzp=i |
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213 | goto 6 |
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214 | endif |
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215 | end do |
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216 | 6 continue |
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217 | |
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218 | ! Vertical distance to the level below and above current position |
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219 | !**************************************************************** |
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220 | |
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221 | dz1=zcolumn_we(k,jy,j)-height(indz) |
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222 | dz2=height(indzp)-zcolumn_we(k,jy,j) |
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223 | dz=1./(dz1+dz2) |
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224 | |
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225 | ! Vertical and temporal interpolation |
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226 | !************************************ |
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227 | |
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228 | do m=1,2 |
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229 | indexh=memind(m) |
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230 | do in=1,2 |
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231 | indzh=indz+in-1 |
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232 | windl(in)=uu(nx_we(k),jy,indzh,indexh) |
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233 | rhol(in)=rho(nx_we(k),jy,indzh,indexh) |
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234 | end do |
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235 | |
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236 | windhl(m)=(dz2*windl(1)+dz1*windl(2))*dz |
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237 | rhohl(m)=(dz2*rhol(1)+dz1*rhol(2))*dz |
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238 | end do |
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239 | |
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240 | windx=(windhl(1)*dt2+windhl(2)*dt1)*dtt |
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241 | rhox=(rhohl(1)*dt2+rhohl(2)*dt1)*dtt |
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242 | |
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243 | ! Calculate mass flux |
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244 | !******************** |
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245 | |
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246 | fluxofmass=windx*rhox*boundarea*real(lsynctime) |
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247 | |
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248 | |
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249 | ! If the mass flux is directed into the domain, add it to previous mass fluxes; |
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250 | ! if it is out of the domain, set accumulated mass flux to zero |
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251 | !****************************************************************************** |
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252 | |
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253 | if (k.eq.1) then |
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254 | if (fluxofmass.ge.0.) then |
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255 | acc_mass_we(k,jy,j)=acc_mass_we(k,jy,j)+fluxofmass |
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256 | else |
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257 | acc_mass_we(k,jy,j)=0. |
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258 | endif |
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259 | else |
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260 | if (fluxofmass.le.0.) then |
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261 | acc_mass_we(k,jy,j)=acc_mass_we(k,jy,j)+abs(fluxofmass) |
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262 | else |
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263 | acc_mass_we(k,jy,j)=0. |
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264 | endif |
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265 | endif |
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266 | accmasst=accmasst+acc_mass_we(k,jy,j) |
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267 | |
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268 | ! If the accumulated mass exceeds half the mass that each particle shall carry, |
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269 | ! one (or more) particle(s) is (are) released and the accumulated mass is |
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270 | ! reduced by the mass of this (these) particle(s) |
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271 | !****************************************************************************** |
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272 | |
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273 | if (acc_mass_we(k,jy,j).ge.xmassperparticle/2.) then |
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274 | mmass=int((acc_mass_we(k,jy,j)+xmassperparticle/2.)/ & |
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275 | xmassperparticle) |
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276 | acc_mass_we(k,jy,j)=acc_mass_we(k,jy,j)- & |
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277 | real(mmass)*xmassperparticle |
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278 | else |
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279 | mmass=0 |
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280 | endif |
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281 | |
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282 | do m=1,mmass |
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283 | do ipart=minpart,maxpart |
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284 | |
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285 | ! If a vacant storage space is found, attribute everything to this array element |
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286 | ! TODO: for the MPI version this test can be removed, as all |
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287 | ! elements in _tmp arrays are initialized to zero |
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288 | !***************************************************************************** |
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289 | |
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290 | if (itra1_tmp(ipart).ne.itime) then |
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291 | |
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292 | ! Assign particle positions |
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293 | !************************** |
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294 | |
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295 | xtra1_tmp(ipart)=real(nx_we(k)) |
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296 | if (jy.eq.ny_sn(1)) then |
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297 | ytra1_tmp(ipart)=real(jy)+0.5*ran1(idummy) |
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298 | else if (jy.eq.ny_sn(2)) then |
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299 | ytra1_tmp(ipart)=real(jy)-0.5*ran1(idummy) |
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300 | else |
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301 | ytra1_tmp(ipart)=real(jy)+(ran1(idummy)-.5) |
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302 | endif |
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303 | if (j.eq.1) then |
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304 | ztra1_tmp(ipart)=zcolumn_we(k,jy,1)+(zcolumn_we(k,jy,2)- & |
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305 | zcolumn_we(k,jy,1))/4. |
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306 | else if (j.eq.numcolumn_we(k,jy)) then |
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307 | ztra1_tmp(ipart)=(2.*zcolumn_we(k,jy,j)+ & |
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308 | zcolumn_we(k,jy,j-1)+height(nz))/4. |
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309 | else |
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310 | ztra1_tmp(ipart)=zcolumn_we(k,jy,j-1)+ran1(idummy)* & |
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311 | (zcolumn_we(k,jy,j+1)-zcolumn_we(k,jy,j-1)) |
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312 | endif |
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313 | |
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314 | ! Interpolate PV to the particle position |
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315 | !**************************************** |
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316 | ixm=int(xtra1_tmp(ipart)) |
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317 | jym=int(ytra1_tmp(ipart)) |
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318 | ixp=ixm+1 |
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319 | jyp=jym+1 |
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320 | ddx=xtra1_tmp(ipart)-real(ixm) |
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321 | ddy=ytra1_tmp(ipart)-real(jym) |
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322 | rddx=1.-ddx |
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323 | rddy=1.-ddy |
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324 | p1=rddx*rddy |
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325 | p2=ddx*rddy |
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326 | p3=rddx*ddy |
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327 | p4=ddx*ddy |
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328 | do i=2,nz |
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329 | if (height(i).gt.ztra1_tmp(ipart)) then |
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330 | indzm=i-1 |
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331 | indzp=i |
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332 | goto 26 |
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333 | endif |
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334 | end do |
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335 | 26 continue |
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336 | dz1=ztra1_tmp(ipart)-height(indzm) |
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337 | dz2=height(indzp)-ztra1_tmp(ipart) |
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338 | dz=1./(dz1+dz2) |
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339 | do mm=1,2 |
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340 | indexh=memind(mm) |
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341 | do in=1,2 |
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342 | indzh=indzm+in-1 |
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343 | y1(in)=p1*pv(ixm,jym,indzh,indexh) & |
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344 | +p2*pv(ixp,jym,indzh,indexh) & |
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345 | +p3*pv(ixm,jyp,indzh,indexh) & |
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346 | +p4*pv(ixp,jyp,indzh,indexh) |
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347 | end do |
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348 | yh1(mm)=(dz2*y1(1)+dz1*y1(2))*dz |
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349 | end do |
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350 | pvpart=(yh1(1)*dt2+yh1(2)*dt1)*dtt |
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351 | ylat=ylat0+ytra1_tmp(ipart)*dy |
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352 | if (ylat.lt.0.) pvpart=-1.*pvpart |
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353 | |
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354 | |
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355 | ! For domain-filling option 2 (stratospheric O3), do the rest only in the stratosphere |
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356 | !***************************************************************************** |
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357 | |
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358 | if (((ztra1_tmp(ipart).gt.3000.).and. & |
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359 | (pvpart.gt.pvcrit)).or.(mdomainfill.eq.1)) then |
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360 | nclass_tmp(ipart)=min(int(ran1(idummy)* & |
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361 | real(nclassunc))+1,nclassunc) |
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362 | numactiveparticles=numactiveparticles+1 |
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363 | numparticlecount=numparticlecount+1 |
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364 | npoint_tmp(ipart)=numparticlecount |
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365 | idt_tmp(ipart)=mintime |
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366 | itra1_tmp(ipart)=itime |
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367 | itramem_tmp(ipart)=itra1_tmp(ipart) |
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368 | itrasplit_tmp(ipart)=itra1_tmp(ipart)+ldirect*itsplit |
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369 | xmass1_tmp(ipart,1)=xmassperparticle |
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370 | if (mdomainfill.eq.2) xmass1_tmp(ipart,1)= & |
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371 | xmass1_tmp(ipart,1)*pvpart*48./29.*ozonescale/10.**9 |
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372 | else |
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373 | goto 71 |
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374 | endif |
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375 | |
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376 | |
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377 | ! Increase numpart, if necessary |
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378 | !******************************* |
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379 | |
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380 | numpart_total=max(numpart_total,ipart) |
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381 | goto 73 ! Storage space has been found, stop searching |
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382 | endif |
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383 | end do |
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384 | if (ipart.gt.tmp_size) & |
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385 | stop 'boundcond_domainfill_mpi.f90: too many particles required' |
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386 | 73 minpart=ipart+1 |
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387 | 71 continue |
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388 | end do |
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389 | |
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390 | |
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391 | end do |
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392 | end do |
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393 | end do |
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394 | |
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395 | |
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396 | !***************************************** |
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397 | ! Southern and northern boundary condition |
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398 | !***************************************** |
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399 | |
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400 | ! Loop from west to east |
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401 | !*********************** |
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402 | |
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403 | do ix=nx_we(1),nx_we(2) |
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404 | |
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405 | ! Loop over southern (index 1) and northern (index 2) boundary |
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406 | !************************************************************* |
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407 | |
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408 | do k=1,2 |
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409 | ylat=ylat0+real(ny_sn(k))*dy |
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410 | cosfact=cos(ylat*pi180) |
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411 | |
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412 | ! Loop over all release locations in a column |
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413 | !******************************************** |
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414 | |
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415 | do j=1,numcolumn_sn(k,ix) |
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416 | |
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417 | ! Determine, for each release location, the area of the corresponding boundary |
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418 | !***************************************************************************** |
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419 | |
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420 | if (j.eq.1) then |
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421 | deltaz=(zcolumn_sn(k,ix,2)+zcolumn_sn(k,ix,1))/2. |
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422 | else if (j.eq.numcolumn_sn(k,ix)) then |
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423 | ! deltaz=height(nz)-(zcolumn_sn(k,ix,j-1)+ |
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424 | ! + zcolumn_sn(k,ix,j))/2. |
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425 | ! In order to avoid taking a very high column for very many particles, |
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426 | ! use the deltaz from one particle below instead |
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427 | deltaz=(zcolumn_sn(k,ix,j)-zcolumn_sn(k,ix,j-2))/2. |
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428 | else |
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429 | deltaz=(zcolumn_sn(k,ix,j+1)-zcolumn_sn(k,ix,j-1))/2. |
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430 | endif |
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431 | if ((ix.eq.nx_we(1)).or.(ix.eq.nx_we(2))) then |
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432 | boundarea=deltaz*111198.5/2.*cosfact*dx |
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433 | else |
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434 | boundarea=deltaz*111198.5*cosfact*dx |
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435 | endif |
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436 | |
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437 | |
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438 | ! Interpolate the wind velocity and density to the release location |
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439 | !****************************************************************** |
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440 | |
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441 | ! Determine the model level below the release position |
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442 | !***************************************************** |
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443 | |
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444 | do i=2,nz |
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445 | if (height(i).gt.zcolumn_sn(k,ix,j)) then |
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446 | indz=i-1 |
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447 | indzp=i |
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448 | goto 16 |
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449 | endif |
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450 | end do |
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451 | 16 continue |
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452 | |
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453 | ! Vertical distance to the level below and above current position |
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454 | !**************************************************************** |
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455 | |
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456 | dz1=zcolumn_sn(k,ix,j)-height(indz) |
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457 | dz2=height(indzp)-zcolumn_sn(k,ix,j) |
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458 | dz=1./(dz1+dz2) |
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459 | |
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460 | ! Vertical and temporal interpolation |
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461 | !************************************ |
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462 | |
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463 | do m=1,2 |
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464 | indexh=memind(m) |
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465 | do in=1,2 |
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466 | indzh=indz+in-1 |
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467 | windl(in)=vv(ix,ny_sn(k),indzh,indexh) |
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468 | rhol(in)=rho(ix,ny_sn(k),indzh,indexh) |
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469 | end do |
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470 | |
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471 | windhl(m)=(dz2*windl(1)+dz1*windl(2))*dz |
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472 | rhohl(m)=(dz2*rhol(1)+dz1*rhol(2))*dz |
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473 | end do |
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474 | |
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475 | windx=(windhl(1)*dt2+windhl(2)*dt1)*dtt |
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476 | rhox=(rhohl(1)*dt2+rhohl(2)*dt1)*dtt |
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477 | |
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478 | ! Calculate mass flux |
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479 | !******************** |
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480 | |
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481 | fluxofmass=windx*rhox*boundarea*real(lsynctime) |
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482 | |
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483 | ! If the mass flux is directed into the domain, add it to previous mass fluxes; |
---|
484 | ! if it is out of the domain, set accumulated mass flux to zero |
---|
485 | !****************************************************************************** |
---|
486 | |
---|
487 | if (k.eq.1) then |
---|
488 | if (fluxofmass.ge.0.) then |
---|
489 | acc_mass_sn(k,ix,j)=acc_mass_sn(k,ix,j)+fluxofmass |
---|
490 | else |
---|
491 | acc_mass_sn(k,ix,j)=0. |
---|
492 | endif |
---|
493 | else |
---|
494 | if (fluxofmass.le.0.) then |
---|
495 | acc_mass_sn(k,ix,j)=acc_mass_sn(k,ix,j)+abs(fluxofmass) |
---|
496 | else |
---|
497 | acc_mass_sn(k,ix,j)=0. |
---|
498 | endif |
---|
499 | endif |
---|
500 | accmasst=accmasst+acc_mass_sn(k,ix,j) |
---|
501 | |
---|
502 | ! If the accumulated mass exceeds half the mass that each particle shall carry, |
---|
503 | ! one (or more) particle(s) is (are) released and the accumulated mass is |
---|
504 | ! reduced by the mass of this (these) particle(s) |
---|
505 | !****************************************************************************** |
---|
506 | |
---|
507 | if (acc_mass_sn(k,ix,j).ge.xmassperparticle/2.) then |
---|
508 | mmass=int((acc_mass_sn(k,ix,j)+xmassperparticle/2.)/ & |
---|
509 | xmassperparticle) |
---|
510 | acc_mass_sn(k,ix,j)=acc_mass_sn(k,ix,j)- & |
---|
511 | real(mmass)*xmassperparticle |
---|
512 | else |
---|
513 | mmass=0 |
---|
514 | endif |
---|
515 | |
---|
516 | do m=1,mmass |
---|
517 | do ipart=minpart,maxpart |
---|
518 | |
---|
519 | ! If a vacant storage space is found, attribute everything to this array element |
---|
520 | !***************************************************************************** |
---|
521 | |
---|
522 | if (itra1_tmp(ipart).ne.itime) then |
---|
523 | |
---|
524 | ! Assign particle positions |
---|
525 | !************************** |
---|
526 | |
---|
527 | ytra1_tmp(ipart)=real(ny_sn(k)) |
---|
528 | if (ix.eq.nx_we(1)) then |
---|
529 | xtra1_tmp(ipart)=real(ix)+0.5*ran1(idummy) |
---|
530 | else if (ix.eq.nx_we(2)) then |
---|
531 | xtra1_tmp(ipart)=real(ix)-0.5*ran1(idummy) |
---|
532 | else |
---|
533 | xtra1_tmp(ipart)=real(ix)+(ran1(idummy)-.5) |
---|
534 | endif |
---|
535 | if (j.eq.1) then |
---|
536 | ztra1_tmp(ipart)=zcolumn_sn(k,ix,1)+(zcolumn_sn(k,ix,2)- & |
---|
537 | zcolumn_sn(k,ix,1))/4. |
---|
538 | else if (j.eq.numcolumn_sn(k,ix)) then |
---|
539 | ztra1_tmp(ipart)=(2.*zcolumn_sn(k,ix,j)+ & |
---|
540 | zcolumn_sn(k,ix,j-1)+height(nz))/4. |
---|
541 | else |
---|
542 | ztra1_tmp(ipart)=zcolumn_sn(k,ix,j-1)+ran1(idummy)* & |
---|
543 | (zcolumn_sn(k,ix,j+1)-zcolumn_sn(k,ix,j-1)) |
---|
544 | endif |
---|
545 | |
---|
546 | |
---|
547 | ! Interpolate PV to the particle position |
---|
548 | !**************************************** |
---|
549 | ixm=int(xtra1_tmp(ipart)) |
---|
550 | jym=int(ytra1_tmp(ipart)) |
---|
551 | ixp=ixm+1 |
---|
552 | jyp=jym+1 |
---|
553 | ddx=xtra1_tmp(ipart)-real(ixm) |
---|
554 | ddy=ytra1_tmp(ipart)-real(jym) |
---|
555 | rddx=1.-ddx |
---|
556 | rddy=1.-ddy |
---|
557 | p1=rddx*rddy |
---|
558 | p2=ddx*rddy |
---|
559 | p3=rddx*ddy |
---|
560 | p4=ddx*ddy |
---|
561 | do i=2,nz |
---|
562 | if (height(i).gt.ztra1_tmp(ipart)) then |
---|
563 | indzm=i-1 |
---|
564 | indzp=i |
---|
565 | goto 126 |
---|
566 | endif |
---|
567 | end do |
---|
568 | 126 continue |
---|
569 | dz1=ztra1_tmp(ipart)-height(indzm) |
---|
570 | dz2=height(indzp)-ztra1_tmp(ipart) |
---|
571 | dz=1./(dz1+dz2) |
---|
572 | do mm=1,2 |
---|
573 | indexh=memind(mm) |
---|
574 | do in=1,2 |
---|
575 | indzh=indzm+in-1 |
---|
576 | y1(in)=p1*pv(ixm,jym,indzh,indexh) & |
---|
577 | +p2*pv(ixp,jym,indzh,indexh) & |
---|
578 | +p3*pv(ixm,jyp,indzh,indexh) & |
---|
579 | +p4*pv(ixp,jyp,indzh,indexh) |
---|
580 | end do |
---|
581 | yh1(mm)=(dz2*y1(1)+dz1*y1(2))*dz |
---|
582 | end do |
---|
583 | pvpart=(yh1(1)*dt2+yh1(2)*dt1)*dtt |
---|
584 | if (ylat.lt.0.) pvpart=-1.*pvpart |
---|
585 | |
---|
586 | |
---|
587 | ! For domain-filling option 2 (stratospheric O3), do the rest only in the stratosphere |
---|
588 | !***************************************************************************** |
---|
589 | |
---|
590 | if (((ztra1_tmp(ipart).gt.3000.).and. & |
---|
591 | (pvpart.gt.pvcrit)).or.(mdomainfill.eq.1)) then |
---|
592 | nclass_tmp(ipart)=min(int(ran1(idummy)* & |
---|
593 | real(nclassunc))+1,nclassunc) |
---|
594 | numactiveparticles=numactiveparticles+1 |
---|
595 | numparticlecount=numparticlecount+1 |
---|
596 | npoint_tmp(ipart)=numparticlecount |
---|
597 | idt_tmp(ipart)=mintime |
---|
598 | itra1_tmp(ipart)=itime |
---|
599 | itramem_tmp(ipart)=itra1_tmp(ipart) |
---|
600 | itrasplit_tmp(ipart)=itra1_tmp(ipart)+ldirect*itsplit |
---|
601 | xmass1_tmp(ipart,1)=xmassperparticle |
---|
602 | if (mdomainfill.eq.2) xmass1_tmp(ipart,1)= & |
---|
603 | xmass1_tmp(ipart,1)*pvpart*48./29.*ozonescale/10.**9 |
---|
604 | else |
---|
605 | goto 171 |
---|
606 | endif |
---|
607 | |
---|
608 | |
---|
609 | ! Increase numpart, if necessary |
---|
610 | !******************************* |
---|
611 | numpart_total=max(numpart_total,ipart) |
---|
612 | goto 173 ! Storage space has been found, stop searching |
---|
613 | endif |
---|
614 | end do |
---|
615 | if (ipart.gt.tmp_size) & |
---|
616 | stop 'boundcond_domainfill.f: too many particles required' |
---|
617 | 173 minpart=ipart+1 |
---|
618 | 171 continue |
---|
619 | end do |
---|
620 | |
---|
621 | |
---|
622 | end do |
---|
623 | end do |
---|
624 | end do |
---|
625 | |
---|
626 | |
---|
627 | ! xm=0. |
---|
628 | ! do i=1,numpart_total |
---|
629 | ! if (itra1_tmp(i).eq.itime) xm=xm+xmass1(i,1) |
---|
630 | ! end do |
---|
631 | |
---|
632 | !write(*,*) itime,numactiveparticles,numparticlecount,numpart, |
---|
633 | ! +xm,accmasst,xm+accmasst |
---|
634 | |
---|
635 | end if ! if lroot |
---|
636 | |
---|
637 | ! Distribute the number of particles to be released |
---|
638 | ! ************************************************* |
---|
639 | call MPI_Bcast(numpart_total, 1, MPI_INTEGER, id_root, mp_comm_used, mp_ierr) |
---|
640 | |
---|
641 | do i=0, mp_partgroup_np-1 |
---|
642 | numrel_mpi(i) = numpart_total/mp_partgroup_np |
---|
643 | if (i.lt.mod(numpart_total,mp_partgroup_np)) numrel_mpi(i) = numrel_mpi(i) + 1 |
---|
644 | end do |
---|
645 | |
---|
646 | ! Allocate temporary arrays for receiving processes |
---|
647 | if (.not.lroot) then |
---|
648 | allocate(itra1_tmp(numrel_mpi(mp_partid)),& |
---|
649 | & npoint_tmp(numrel_mpi(mp_partid)),& |
---|
650 | & nclass_tmp(numrel_mpi(mp_partid)),& |
---|
651 | & idt_tmp(numrel_mpi(mp_partid)),& |
---|
652 | & itramem_tmp(numrel_mpi(mp_partid)),& |
---|
653 | & itrasplit_tmp(numrel_mpi(mp_partid)),& |
---|
654 | & xtra1_tmp(numrel_mpi(mp_partid)),& |
---|
655 | & ytra1_tmp(numrel_mpi(mp_partid)),& |
---|
656 | & ztra1_tmp(numrel_mpi(mp_partid)),& |
---|
657 | & xmass1_tmp(numrel_mpi(mp_partid),maxspec)) |
---|
658 | |
---|
659 | ! Initialize all particles as non-existent |
---|
660 | itra1_tmp(:)=-999999999 |
---|
661 | end if |
---|
662 | |
---|
663 | ! Distribute particles |
---|
664 | ! Keep track of released particles so far |
---|
665 | rel_counter = 0 |
---|
666 | mtag = 1000 |
---|
667 | |
---|
668 | do i=0, mp_partgroup_np-1 |
---|
669 | |
---|
670 | ! For root process, nothing to do except update release count |
---|
671 | if (i.eq.0) then |
---|
672 | rel_counter = rel_counter + numrel_mpi(i) |
---|
673 | cycle |
---|
674 | end if |
---|
675 | |
---|
676 | ! Send particles from root to non-root processes |
---|
677 | if (lroot.and.numrel_mpi(i).gt.0) then |
---|
678 | |
---|
679 | call MPI_SEND(nclass_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
680 | &numrel_mpi(i),MPI_INTEGER,i,mtag+1*i,mp_comm_used,mp_ierr) |
---|
681 | |
---|
682 | call MPI_SEND(npoint_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
683 | &numrel_mpi(i),MPI_INTEGER,i,mtag+2*i,mp_comm_used,mp_ierr) |
---|
684 | |
---|
685 | call MPI_SEND(itra1_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
686 | &numrel_mpi(i),MPI_INTEGER,i,mtag+3*i,mp_comm_used,mp_ierr) |
---|
687 | |
---|
688 | call MPI_SEND(idt_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
689 | &numrel_mpi(i),MPI_INTEGER,i,mtag+4*i,mp_comm_used,mp_ierr) |
---|
690 | |
---|
691 | call MPI_SEND(itramem_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
692 | &numrel_mpi(i),MPI_INTEGER,i,mtag+5*i,mp_comm_used,mp_ierr) |
---|
693 | |
---|
694 | call MPI_SEND(itrasplit_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
695 | &numrel_mpi(i),MPI_INTEGER,i,mtag+6*i,mp_comm_used,mp_ierr) |
---|
696 | |
---|
697 | call MPI_SEND(xtra1_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
698 | &numrel_mpi(i),mp_dp,i,mtag+7*i,mp_comm_used,mp_ierr) |
---|
699 | |
---|
700 | call MPI_SEND(ytra1_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
701 | &numrel_mpi(i),mp_dp,i,mtag+8*i,mp_comm_used,mp_ierr) |
---|
702 | |
---|
703 | call MPI_SEND(ztra1_tmp(rel_counter+1:rel_counter+numrel_mpi(i)),& |
---|
704 | &numrel_mpi(i),mp_sp,i,mtag+9*i,mp_comm_used,mp_ierr) |
---|
705 | |
---|
706 | do j=1,nspec |
---|
707 | call MPI_SEND(xmass1_tmp(rel_counter+1:rel_counter+numrel_mpi(i),j),& |
---|
708 | &numrel_mpi(i),mp_sp,i,mtag+(9+j)*i,mp_comm_used,mp_ierr) |
---|
709 | end do |
---|
710 | |
---|
711 | ! Non-root processes issue receive requests |
---|
712 | else if (i.eq.mp_partid.and.numrel_mpi(i).gt.0) then |
---|
713 | call MPI_RECV(nclass_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
714 | &MPI_INTEGER,id_root,mtag+1*i,mp_comm_used,mp_status,mp_ierr) |
---|
715 | |
---|
716 | call MPI_RECV(npoint_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
717 | &MPI_INTEGER,id_root,mtag+2*i,mp_comm_used,mp_status,mp_ierr) |
---|
718 | |
---|
719 | call MPI_RECV(itra1_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
720 | &MPI_INTEGER,id_root,mtag+3*i,mp_comm_used,mp_status,mp_ierr) |
---|
721 | |
---|
722 | call MPI_RECV(idt_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
723 | &MPI_INTEGER,id_root,mtag+4*i,mp_comm_used,mp_status,mp_ierr) |
---|
724 | |
---|
725 | call MPI_RECV(itramem_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
726 | &MPI_INTEGER,id_root,mtag+5*i,mp_comm_used,mp_status,mp_ierr) |
---|
727 | |
---|
728 | call MPI_RECV(itrasplit_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
729 | &MPI_INTEGER,id_root,mtag+6*i,mp_comm_used,mp_status,mp_ierr) |
---|
730 | |
---|
731 | call MPI_RECV(xtra1_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
732 | &mp_dp,id_root,mtag+7*i,mp_comm_used,mp_status,mp_ierr) |
---|
733 | |
---|
734 | call MPI_RECV(ytra1_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
735 | &mp_dp,id_root,mtag+8*i,mp_comm_used,mp_status,mp_ierr) |
---|
736 | |
---|
737 | call MPI_RECV(ztra1_tmp(1:numrel_mpi(i)),numrel_mpi(i),& |
---|
738 | &mp_sp,id_root,mtag+9*i,mp_comm_used,mp_status,mp_ierr) |
---|
739 | |
---|
740 | do j=1,nspec |
---|
741 | call MPI_RECV(xmass1_tmp(1:numrel_mpi(i),j),numrel_mpi(i),& |
---|
742 | &mp_sp,id_root,mtag+(9+j)*i,mp_comm_used,mp_status,mp_ierr) |
---|
743 | |
---|
744 | end do |
---|
745 | end if |
---|
746 | rel_counter = rel_counter + numrel_mpi(i) |
---|
747 | end do |
---|
748 | |
---|
749 | ! Find free storage space for the new particles. |
---|
750 | ! This section is independent of the redistribution scheme used |
---|
751 | ! ******************************************************************** |
---|
752 | |
---|
753 | ! Keep track of released particles so far |
---|
754 | minpart=1 |
---|
755 | |
---|
756 | ! The algorithm should be correct also for root process |
---|
757 | do i=1, numrel_mpi(mp_partid) |
---|
758 | do ipart=minpart, maxpart |
---|
759 | if (itra1(ipart).ne.itime) then |
---|
760 | itra1(ipart) = itra1_tmp(i) |
---|
761 | npoint(ipart) = npoint_tmp(i) |
---|
762 | nclass(ipart) = nclass_tmp(i) |
---|
763 | idt(ipart) = idt_tmp(i) |
---|
764 | itramem(ipart) = itramem_tmp(i) |
---|
765 | itrasplit(ipart) = itrasplit_tmp(i) |
---|
766 | xtra1(ipart) = xtra1_tmp(i) |
---|
767 | ytra1(ipart) = ytra1_tmp(i) |
---|
768 | ztra1(ipart) = ztra1_tmp(i) |
---|
769 | xmass1(ipart,:) = xmass1_tmp(i,:) |
---|
770 | ! Increase numpart, if necessary |
---|
771 | numpart=max(numpart,ipart) |
---|
772 | goto 200 ! Storage space has been found, stop searching |
---|
773 | end if |
---|
774 | end do |
---|
775 | 200 minpart=ipart+1 |
---|
776 | end do |
---|
777 | |
---|
778 | ! If particles shall be dumped, then accumulated masses at the domain boundaries |
---|
779 | ! must be dumped, too, to be used for later runs |
---|
780 | !***************************************************************************** |
---|
781 | |
---|
782 | if ((ipout.gt.0).and.(itime.eq.loutend)) then |
---|
783 | if (lroot) then |
---|
784 | call mpif_mtime('iotime',0) |
---|
785 | open(unitboundcond,file=path(2)(1:length(2))//'boundcond.bin', & |
---|
786 | form='unformatted') |
---|
787 | write(unitboundcond) numcolumn_we,numcolumn_sn, & |
---|
788 | zcolumn_we,zcolumn_sn,acc_mass_we,acc_mass_sn |
---|
789 | close(unitboundcond) |
---|
790 | call mpif_mtime('iotime',1) |
---|
791 | end if |
---|
792 | endif |
---|
793 | |
---|
794 | ! Deallocate temporary arrays |
---|
795 | deallocate(itra1_tmp,npoint_tmp,nclass_tmp,idt_tmp,itramem_tmp,itrasplit_tmp,& |
---|
796 | & xtra1_tmp,ytra1_tmp,ztra1_tmp,xmass1_tmp,numrel_mpi) |
---|
797 | ! numactiveparticles_mpi |
---|
798 | |
---|
799 | |
---|
800 | end subroutine boundcond_domainfill |
---|