1 | SUBROUTINE timestep |
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2 | |
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3 | !------------------------------------------------------------------------------! |
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4 | ! Actual revisions: |
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5 | ! ----------------- |
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6 | ! |
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7 | ! |
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8 | ! Former revisions: |
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9 | ! ----------------- |
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10 | ! $Id: timestep.f90 4 2007-02-13 11:33:16Z raasch $ |
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11 | ! RCS Log replace by Id keyword, revision history cleaned up |
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12 | ! |
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13 | ! Revision 1.21 2006/02/23 12:59:44 raasch |
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14 | ! nt_anz renamed current_timestep_number |
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15 | ! |
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16 | ! Revision 1.1 1997/08/11 06:26:19 raasch |
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17 | ! Initial revision |
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18 | ! |
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19 | ! |
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20 | ! Description: |
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21 | ! ------------ |
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22 | ! Compute the time step under consideration of the FCL and diffusion criterion. |
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23 | !------------------------------------------------------------------------------! |
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24 | |
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25 | USE arrays_3d |
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26 | USE control_parameters |
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27 | USE cpulog |
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28 | USE grid_variables |
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29 | USE indices |
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30 | USE interfaces |
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31 | USE pegrid |
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32 | USE statistics |
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33 | |
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34 | IMPLICIT NONE |
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35 | |
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36 | INTEGER :: i, j, k |
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37 | |
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38 | REAL :: div, dt_diff, dt_diff_l, dt_u, dt_v, dt_w, percent_change, & |
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39 | u_gtrans_l, value, v_gtrans_l |
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40 | |
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41 | REAL, DIMENSION(2) :: uv_gtrans, uv_gtrans_l |
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42 | REAL, DIMENSION(nzb+1:nzt) :: dxyz2_min |
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43 | |
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44 | |
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45 | CALL cpu_log( log_point(12), 'calculate_timestep', 'start' ) |
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46 | |
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47 | ! |
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48 | !-- Determine the maxima of the velocity components. |
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49 | CALL global_min_max( nzb, nzt+1, nys-1, nyn+1, nxl-1, nxr+1, u, 'abs', & |
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50 | u_max, u_max_ijk ) |
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51 | CALL global_min_max( nzb, nzt+1, nys-1, nyn+1, nxl-1, nxr+1, v, 'abs', & |
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52 | v_max, v_max_ijk ) |
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53 | CALL global_min_max( nzb, nzt+1, nys-1, nyn+1, nxl-1, nxr+1, w, 'abs', & |
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54 | w_max, w_max_ijk ) |
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55 | |
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56 | ! |
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57 | !-- In case maxima of the horizontal velocity components have been found at the |
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58 | !-- bottom boundary (k=nzb), the corresponding maximum at level k=1 is chosen |
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59 | !-- if the Dirichlet-boundary condition ('mirror') has been set. This is |
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60 | !-- necessary, because otherwise in case of Galilei-transform a far too large |
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61 | !-- velocity (having the respective opposite sign) would be used for the time |
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62 | !-- step determination (almost double the mean flow velocity). |
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63 | IF ( ibc_uv_b == 0 ) THEN |
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64 | IF ( u_max_ijk(1) == nzb ) THEN |
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65 | u_max = -u_max |
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66 | u_max_ijk(1) = nzb + 1 |
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67 | ENDIF |
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68 | IF ( v_max_ijk(1) == nzb ) THEN |
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69 | v_max = -v_max |
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70 | v_max_ijk(1) = nzb + 1 |
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71 | ENDIF |
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72 | ENDIF |
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73 | |
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74 | ! |
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75 | !-- In case of Galilei-transform not using the geostrophic wind as translation |
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76 | !-- velocity, compute the volume-averaged horizontal velocity components, which |
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77 | !-- will then be subtracted from the horizontal wind for the time step and |
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78 | !-- horizontal advection routines. |
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79 | IF ( galilei_transformation .AND. .NOT. use_ug_for_galilei_tr ) THEN |
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80 | IF ( flow_statistics_called ) THEN |
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81 | ! |
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82 | !-- Horizontal averages already existent, just need to average them |
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83 | !-- vertically. |
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84 | u_gtrans = 0.0 |
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85 | v_gtrans = 0.0 |
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86 | DO k = nzb+1, nzt |
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87 | u_gtrans = u_gtrans + hom(k,1,1,0) |
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88 | v_gtrans = v_gtrans + hom(k,1,2,0) |
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89 | ENDDO |
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90 | u_gtrans = u_gtrans / REAL( nzt - nzb ) |
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91 | v_gtrans = v_gtrans / REAL( nzt - nzb ) |
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92 | ELSE |
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93 | ! |
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94 | !-- Averaging over the entire model domain. |
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95 | uv_gtrans_l = 0.0 |
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96 | DO i = nxl, nxr |
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97 | DO j = nys, nyn |
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98 | DO k = nzb+1, nzt |
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99 | uv_gtrans_l(1) = uv_gtrans_l(1) + u(k,j,i) |
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100 | uv_gtrans_l(2) = uv_gtrans_l(2) + v(k,j,i) |
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101 | ENDDO |
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102 | ENDDO |
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103 | ENDDO |
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104 | uv_gtrans_l = uv_gtrans_l / REAL( (nxr-nxl+1)*(nyn-nys+1)*(nzt-nzb) ) |
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105 | #if defined( __parallel ) |
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106 | CALL MPI_ALLREDUCE( uv_gtrans_l, uv_gtrans, 2, MPI_REAL, MPI_SUM, & |
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107 | comm2d, ierr ) |
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108 | u_gtrans = uv_gtrans(1) / REAL( numprocs ) |
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109 | v_gtrans = uv_gtrans(2) / REAL( numprocs ) |
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110 | #else |
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111 | u_gtrans = uv_gtrans_l(1) |
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112 | v_gtrans = uv_gtrans_l(2) |
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113 | #endif |
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114 | ENDIF |
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115 | ENDIF |
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116 | |
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117 | IF ( .NOT. dt_fixed ) THEN |
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118 | ! |
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119 | !-- Variable time step: |
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120 | ! |
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121 | !-- For each component, compute the maximum time step according to the |
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122 | !-- FCL-criterion. |
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123 | dt_u = dx / ( ABS( u_max - u_gtrans ) + 1.0E-10 ) |
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124 | dt_v = dy / ( ABS( v_max - v_gtrans ) + 1.0E-10 ) |
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125 | dt_w = dzu(MAX( 1, w_max_ijk(1) )) / ( ABS( w_max ) + 1.0E-10 ) |
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126 | |
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127 | ! |
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128 | !-- Compute time step according to the diffusion criterion. |
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129 | !-- First calculate minimum grid spacing which only depends on index k |
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130 | !-- Note: also at k=nzb+1 a full grid length is being assumed, although |
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131 | !-- in the Prandtl-layer friction term only dz/2 is used. |
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132 | !-- Experience from the old model seems to justify this. |
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133 | dt_diff_l = 999999.0 |
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134 | |
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135 | DO k = nzb+1, nzt |
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136 | dxyz2_min(k) = MIN( dx2, dy2, dzu(k)*dzu(k) ) * 0.125 |
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137 | ENDDO |
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138 | |
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139 | !$OMP PARALLEL private(i,j,k,value) reduction(MIN: dt_diff_l) |
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140 | !$OMP DO |
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141 | DO i = nxl, nxr |
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142 | DO j = nys, nyn |
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143 | DO k = nzb+1, nzt |
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144 | value = dxyz2_min(k) / ( MAX( kh(k,j,i), km(k,j,i) ) + 1E-20 ) |
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145 | |
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146 | dt_diff_l = MIN( value, dt_diff_l ) |
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147 | ENDDO |
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148 | ENDDO |
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149 | ENDDO |
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150 | !$OMP END PARALLEL |
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151 | #if defined( __parallel ) |
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152 | CALL MPI_ALLREDUCE( dt_diff_l, dt_diff, 1, MPI_REAL, MPI_MIN, comm2d, & |
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153 | ierr ) |
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154 | #else |
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155 | dt_diff = dt_diff_l |
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156 | #endif |
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157 | |
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158 | ! |
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159 | !-- In case of non-cyclic lateral boundaries, the diffusion time step |
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160 | !-- may be further restricted by the lateral damping layer (damping only |
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161 | !-- along x and y) |
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162 | IF ( bc_lr /= 'cyclic' ) THEN |
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163 | dt_diff = MIN( dt_diff, 0.125 * dx2 / ( km_damp_max + 1E-20 ) ) |
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164 | ELSEIF ( bc_ns /= 'cyclic' ) THEN |
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165 | dt_diff = MIN( dt_diff, 0.125 * dy2 / ( km_damp_max + 1E-20 ) ) |
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166 | ENDIF |
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167 | |
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168 | ! |
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169 | !-- The time step is the minimum of the 3 components and the diffusion time |
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170 | !-- step minus a reduction to be on the safe side. Factor 0.5 is necessary |
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171 | !-- since the leap-frog scheme always progresses by 2 * delta t. |
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172 | !-- The user has to set the cfl_factor small enough to ensure that the |
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173 | !-- divergences do not become too large. |
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174 | !-- The time step must not exceed the maximum allowed value. |
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175 | IF ( timestep_scheme(1:5) == 'runge' ) THEN |
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176 | dt_3d = cfl_factor * MIN( dt_diff, dt_u, dt_v, dt_w ) |
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177 | ELSE |
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178 | dt_3d = cfl_factor * 0.5 * MIN( dt_diff, dt_u, dt_v, dt_w ) |
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179 | ENDIF |
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180 | dt_3d = MIN( dt_3d, dt_max ) |
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181 | |
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182 | ! |
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183 | !-- Remember the restricting time step criterion for later output. |
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184 | IF ( dt_diff > MIN( dt_u, dt_v, dt_w ) ) THEN |
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185 | timestep_reason = 'A' |
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186 | ELSE |
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187 | timestep_reason = 'D' |
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188 | ENDIF |
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189 | |
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190 | ! |
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191 | !-- Set flag if the time step becomes too small. |
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192 | IF ( dt_3d < ( 0.00001 * dt_max ) ) THEN |
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193 | stop_dt = .TRUE. |
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194 | IF ( myid == 0 ) THEN |
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195 | PRINT*,'+++ time_step: Time step has reached minimum limit.' |
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196 | PRINT*,' dt = ', dt_3d, ' s Simulation is terminated.' |
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197 | PRINT*,' old_dt = ', old_dt, ' s' |
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198 | PRINT*,' dt_u = ', dt_u, ' s' |
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199 | PRINT*,' dt_v = ', dt_v, ' s' |
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200 | PRINT*,' dt_w = ', dt_w, ' s' |
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201 | PRINT*,' dt_diff = ', dt_diff, ' s' |
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202 | PRINT*,' u_max = ', u_max, ' m/s k=', u_max_ijk(1), & |
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203 | ' j=', u_max_ijk(2), ' i=', u_max_ijk(3) |
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204 | PRINT*,' v_max = ', v_max, ' m/s k=', v_max_ijk(1), & |
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205 | ' j=', v_max_ijk(2), ' i=', v_max_ijk(3) |
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206 | PRINT*,' w_max = ', w_max, ' m/s k=', w_max_ijk(1), & |
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207 | ' j=', w_max_ijk(2), ' i=', w_max_ijk(3) |
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208 | ENDIF |
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209 | ENDIF |
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210 | |
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211 | ! |
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212 | !-- Ensure a smooth value (two significant digits) of the timestep. For |
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213 | !-- other schemes than Runge-Kutta, the following restrictions appear: |
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214 | !-- The current timestep is only then changed, if the change relative to |
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215 | !-- its previous value exceeds +5 % or -2 %. In case of a timestep |
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216 | !-- reduction, at least 30 iterations have to be performed before a timestep |
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217 | !-- enlargement is permitted again. |
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218 | percent_change = dt_3d / old_dt - 1.0 |
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219 | IF ( percent_change > 0.05 .OR. percent_change < -0.02 .OR. & |
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220 | timestep_scheme(1:5) == 'runge' ) THEN |
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221 | |
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222 | ! |
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223 | !-- Time step enlargement by no more than 2 %. |
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224 | IF ( percent_change > 0.0 .AND. simulated_time /= 0.0 .AND. & |
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225 | timestep_scheme(1:5) /= 'runge' ) THEN |
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226 | dt_3d = 1.02 * old_dt |
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227 | ENDIF |
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228 | |
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229 | ! |
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230 | !-- A relatively smooth value of the time step is ensured by taking |
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231 | !-- only the first two significant digits. |
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232 | div = 1000.0 |
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233 | DO WHILE ( dt_3d < div ) |
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234 | div = div / 10.0 |
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235 | ENDDO |
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236 | dt_3d = NINT( dt_3d * 100.0 / div ) * div / 100.0 |
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237 | |
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238 | ! |
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239 | !-- Now the time step can be adjusted. |
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240 | IF ( percent_change < 0.0 .OR. timestep_scheme(1:5) == 'runge' ) & |
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241 | THEN |
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242 | ! |
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243 | !-- Time step reduction. |
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244 | old_dt = dt_3d |
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245 | dt_changed = .TRUE. |
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246 | ELSE |
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247 | ! |
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248 | !-- For other timestep schemes , the time step is only enlarged |
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249 | !-- after at least 30 iterations since the previous time step |
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250 | !-- change or, of course, after model initialization. |
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251 | IF ( current_timestep_number >= last_dt_change + 30 .OR. & |
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252 | simulated_time == 0.0 ) THEN |
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253 | old_dt = dt_3d |
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254 | dt_changed = .TRUE. |
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255 | ELSE |
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256 | dt_3d = old_dt |
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257 | dt_changed = .FALSE. |
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258 | ENDIF |
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259 | |
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260 | ENDIF |
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261 | ELSE |
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262 | ! |
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263 | !-- No time step change since the difference is too small. |
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264 | dt_3d = old_dt |
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265 | dt_changed = .FALSE. |
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266 | ENDIF |
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267 | |
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268 | IF ( dt_changed ) last_dt_change = current_timestep_number |
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269 | |
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270 | ENDIF |
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271 | |
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272 | CALL cpu_log( log_point(12), 'calculate_timestep', 'stop' ) |
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273 | |
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274 | |
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275 | END SUBROUTINE timestep |
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