1 | MODULE dynadv_ubs |
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2 | !!====================================================================== |
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3 | !! *** MODULE dynadv_ubs *** |
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4 | !! Ocean dynamics: Update the momentum trend with the flux form advection |
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5 | !! trend using a 3rd order upstream biased scheme |
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6 | !!====================================================================== |
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7 | !! History : 2.0 ! 2006-08 (R. Benshila, L. Debreu) Original code |
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8 | !! 3.2 ! 2009-07 (R. Benshila) Suppression of rigid-lid option |
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9 | !!---------------------------------------------------------------------- |
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10 | |
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11 | !!---------------------------------------------------------------------- |
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12 | !! dyn_adv_ubs : flux form momentum advection using (ln_dynadv=T) |
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13 | !! an 3rd order Upstream Biased Scheme or Quick scheme |
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14 | !! combined with 2nd or 4th order finite differences |
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15 | !!---------------------------------------------------------------------- |
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16 | USE oce ! ocean dynamics and tracers |
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17 | USE dom_oce ! ocean space and time domain |
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18 | USE trd_oce ! trends: ocean variables |
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19 | USE trddyn ! trend manager: dynamics |
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20 | ! |
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21 | USE in_out_manager ! I/O manager |
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22 | USE prtctl ! Print control |
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23 | USE lbclnk ! ocean lateral boundary conditions (or mpp link) |
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24 | USE lib_mpp ! MPP library |
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25 | |
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26 | IMPLICIT NONE |
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27 | PRIVATE |
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28 | |
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29 | REAL(wp), PARAMETER :: gamma1 = 1._wp/3._wp ! =1/4 quick ; =1/3 3rd order UBS |
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30 | REAL(wp), PARAMETER :: gamma2 = 1._wp/32._wp ! =0 2nd order ; =1/32 4th order centred |
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31 | |
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32 | PUBLIC dyn_adv_ubs ! routine called by step.F90 |
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33 | |
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34 | !! * Substitutions |
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35 | # include "do_loop_substitute.h90" |
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36 | # include "domzgr_substitute.h90" |
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37 | !!---------------------------------------------------------------------- |
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38 | !! NEMO/OCE 4.0 , NEMO Consortium (2018) |
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39 | !! $Id$ |
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40 | !! Software governed by the CeCILL license (see ./LICENSE) |
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41 | !!---------------------------------------------------------------------- |
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42 | CONTAINS |
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43 | |
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44 | SUBROUTINE dyn_adv_ubs( kt, Kbb, Kmm, puu, pvv, Krhs, pau, pav, paw, no_zad ) |
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45 | !!---------------------------------------------------------------------- |
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46 | !! *** ROUTINE dyn_adv_ubs *** |
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47 | !! |
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48 | !! ** Purpose : Compute the now momentum advection trend in flux form |
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49 | !! and the general trend of the momentum equation. |
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50 | !! |
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51 | !! ** Method : The scheme is the one implemeted in ROMS. It depends |
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52 | !! on two parameter gamma1 and gamma2. The former control the |
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53 | !! upstream baised part of the scheme and the later the centred |
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54 | !! part: gamma1 = 0 pure centered (no diffusive part) |
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55 | !! = 1/4 Quick scheme |
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56 | !! = 1/3 3rd order Upstream biased scheme |
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57 | !! gamma2 = 0 2nd order finite differencing |
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58 | !! = 1/32 4th order finite differencing |
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59 | !! For stability reasons, the first term of the fluxes which cor- |
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60 | !! responds to a second order centered scheme is evaluated using |
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61 | !! the now velocity (centered in time) while the second term which |
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62 | !! is the diffusive part of the scheme, is evaluated using the |
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63 | !! before velocity (forward in time). |
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64 | !! Default value (hard coded in the begining of the module) are |
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65 | !! gamma1=1/3 and gamma2=1/32. |
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66 | !! |
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67 | !! In RK3 time stepping case, the optional arguments |
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68 | !! (pau,pav,paw) are present. They are used as advective velocity |
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69 | !! while the advected velocity remains (puu,pvv). |
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70 | !! |
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71 | !! ** Action : (puu,pvv)(:,:,:,Krhs) updated with the advective trend |
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72 | !! |
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73 | !! Reference : Shchepetkin & McWilliams, 2005, Ocean Modelling. |
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74 | !!---------------------------------------------------------------------- |
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75 | INTEGER , INTENT(in ) :: kt , Kbb, Kmm, Krhs ! ocean time-step and level indices |
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76 | INTEGER , OPTIONAL , INTENT(in ) :: no_zad ! no vertical advection compotation |
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77 | REAL(wp), DIMENSION(jpi,jpj,jpk,jpt), TARGET, INTENT(inout) :: puu, pvv ! ocean velocities and RHS of momentum equation |
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78 | REAL(wp), DIMENSION(:,:,:), OPTIONAL, TARGET, INTENT(in ) :: pau, pav, paw ! advective velocity |
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79 | ! |
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80 | INTEGER :: ji, jj, jk ! dummy loop indices |
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81 | REAL(wp) :: zui, zvj, zfuj, zfvi, zl_u, zl_v, zzu, zzv ! local scalars |
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82 | REAL(wp), DIMENSION(A2D(nn_hls),jpk) :: zfu_t, zfu_f, zfu_uw, zfu |
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83 | REAL(wp), DIMENSION(A2D(nn_hls),jpk) :: zfv_t, zfv_f, zfv_vw, zfv, zfw |
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84 | REAL(wp), DIMENSION(A2D(nn_hls),jpk,2) :: zlu_uu, zlu_uv |
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85 | REAL(wp), DIMENSION(A2D(nn_hls),jpk,2) :: zlv_vv, zlv_vu |
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86 | REAL(wp), DIMENSION(:,:,:), POINTER :: zpt_u, zpt_v, zpt_w |
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87 | !!---------------------------------------------------------------------- |
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88 | ! |
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89 | IF( .NOT. l_istiled .OR. ntile == 1 ) THEN ! Do only on the first tile |
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90 | IF( kt == nit000 ) THEN |
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91 | IF(lwp) WRITE(numout,*) |
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92 | IF(lwp) WRITE(numout,*) 'dyn_adv_ubs : UBS flux form momentum advection' |
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93 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~~' |
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94 | ENDIF |
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95 | ENDIF |
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96 | ! |
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97 | zfu_t(:,:,:) = 0._wp |
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98 | zfv_t(:,:,:) = 0._wp |
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99 | zfu_f(:,:,:) = 0._wp |
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100 | zfv_f(:,:,:) = 0._wp |
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101 | ! |
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102 | zlu_uu(:,:,:,:) = 0._wp |
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103 | zlv_vv(:,:,:,:) = 0._wp |
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104 | zlu_uv(:,:,:,:) = 0._wp |
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105 | zlv_vu(:,:,:,:) = 0._wp |
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106 | ! |
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107 | IF( l_trddyn ) THEN ! trends: store the input trends |
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108 | zfu_uw(:,:,:) = puu(:,:,:,Krhs) |
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109 | zfv_vw(:,:,:) = pvv(:,:,:,Krhs) |
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110 | ENDIF |
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111 | ! |
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112 | IF( PRESENT( pau ) ) THEN ! RK3: advective velocity (pau,pav,paw) /= advected velocity (puu,pvv,ww) |
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113 | zpt_u => pau(:,:,:) |
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114 | zpt_v => pav(:,:,:) |
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115 | zpt_w => paw(:,:,:) |
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116 | ELSE ! MLF: advective velocity = (puu,pvv,ww) |
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117 | zpt_u => puu(:,:,:,Kmm) |
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118 | zpt_v => pvv(:,:,:,Kmm) |
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119 | zpt_w => ww (:,:,: ) |
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120 | ENDIF |
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121 | ! |
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122 | ! ! =========================== ! |
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123 | DO jk = 1, jpkm1 ! Laplacian of the velocity ! |
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124 | ! ! =========================== ! |
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125 | ! ! horizontal volume fluxes |
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126 | DO_2D( nn_hls, nn_hls, nn_hls, nn_hls ) |
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127 | zfu(ji,jj,jk) = e2u(ji,jj) * e3u(ji,jj,jk,Kmm) * zpt_u(ji,jj,jk) |
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128 | zfv(ji,jj,jk) = e1v(ji,jj) * e3v(ji,jj,jk,Kmm) * zpt_v(ji,jj,jk) |
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129 | END_2D |
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130 | ! |
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131 | DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 ) ! laplacian |
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132 | ! round brackets added to fix the order of floating point operations |
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133 | ! needed to ensure halo 1 - halo 2 compatibility |
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134 | zlu_uu(ji,jj,jk,1) = ( ( puu (ji+1,jj ,jk,Kbb) - puu (ji ,jj ,jk,Kbb) & |
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135 | & ) & ! bracket for halo 1 - halo 2 compatibility |
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136 | & + ( puu (ji-1,jj ,jk,Kbb) - puu (ji ,jj ,jk,Kbb) & |
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137 | & ) & ! bracket for halo 1 - halo 2 compatibility |
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138 | & ) * umask(ji ,jj ,jk) |
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139 | zlv_vv(ji,jj,jk,1) = ( ( pvv (ji ,jj+1,jk,Kbb) - pvv (ji ,jj ,jk,Kbb) & |
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140 | & ) & ! bracket for halo 1 - halo 2 compatibility |
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141 | & + ( pvv (ji ,jj-1,jk,Kbb) - pvv (ji ,jj ,jk,Kbb) & |
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142 | & ) & ! bracket for halo 1 - halo 2 compatibility |
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143 | & ) * vmask(ji ,jj ,jk) |
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144 | zlu_uv(ji,jj,jk,1) = ( puu (ji ,jj+1,jk,Kbb) - puu (ji ,jj ,jk,Kbb) ) * fmask(ji ,jj ,jk) & |
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145 | & - ( puu (ji ,jj ,jk,Kbb) - puu (ji ,jj-1,jk,Kbb) ) * fmask(ji ,jj-1,jk) |
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146 | zlv_vu(ji,jj,jk,1) = ( pvv (ji+1,jj ,jk,Kbb) - pvv (ji ,jj ,jk,Kbb) ) * fmask(ji ,jj ,jk) & |
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147 | & - ( pvv (ji ,jj ,jk,Kbb) - pvv (ji-1,jj ,jk,Kbb) ) * fmask(ji-1,jj ,jk) |
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148 | ! |
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149 | ! round brackets added to fix the order of floating point operations |
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150 | ! needed to ensure halo 1 - halo 2 compatibility |
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151 | zlu_uu(ji,jj,jk,2) = ( ( zfu(ji+1,jj ,jk) - zfu(ji ,jj ,jk) & |
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152 | & ) & ! bracket for halo 1 - halo 2 compatibility |
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153 | & + ( zfu(ji-1,jj ,jk) - zfu(ji ,jj ,jk) & |
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154 | & ) & ! bracket for halo 1 - halo 2 compatibility |
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155 | & ) * umask(ji ,jj ,jk) |
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156 | zlv_vv(ji,jj,jk,2) = ( ( zfv(ji ,jj+1,jk) - zfv(ji ,jj ,jk) & |
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157 | & ) & ! bracket for halo 1 - halo 2 compatibility |
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158 | & + ( zfv(ji ,jj-1,jk) - zfv(ji ,jj ,jk) & |
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159 | & ) & ! bracket for halo 1 - halo 2 compatibility |
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160 | & ) * vmask(ji ,jj ,jk) |
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161 | zlu_uv(ji,jj,jk,2) = ( zfu(ji ,jj+1,jk) - zfu(ji ,jj ,jk) ) * fmask(ji ,jj ,jk) & |
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162 | & - ( zfu(ji ,jj ,jk) - zfu(ji ,jj-1,jk) ) * fmask(ji ,jj-1,jk) |
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163 | zlv_vu(ji,jj,jk,2) = ( zfv(ji+1,jj ,jk) - zfv(ji ,jj ,jk) ) * fmask(ji ,jj ,jk) & |
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164 | & - ( zfv(ji ,jj ,jk) - zfv(ji-1,jj ,jk) ) * fmask(ji-1,jj ,jk) |
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165 | END_2D |
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166 | END DO |
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167 | IF( nn_hls == 1 ) CALL lbc_lnk( 'dynadv_ubs', zlu_uu(:,:,:,1), 'U', -1.0_wp , zlu_uv(:,:,:,1), 'U', -1.0_wp, & |
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168 | & zlu_uu(:,:,:,2), 'U', -1.0_wp , zlu_uv(:,:,:,2), 'U', -1.0_wp, & |
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169 | & zlv_vv(:,:,:,1), 'V', -1.0_wp , zlv_vu(:,:,:,1), 'V', -1.0_wp, & |
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170 | & zlv_vv(:,:,:,2), 'V', -1.0_wp , zlv_vu(:,:,:,2), 'V', -1.0_wp ) |
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171 | ! |
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172 | ! ! ====================== ! |
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173 | ! ! Horizontal advection ! |
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174 | DO jk = 1, jpkm1 ! ====================== ! |
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175 | ! ! horizontal volume fluxes |
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176 | DO_2D( 1, 1, 1, 1 ) |
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177 | zfu(ji,jj,jk) = 0.25_wp * e2u(ji,jj) * e3u(ji,jj,jk,Kmm) * zpt_u(ji,jj,jk) |
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178 | zfv(ji,jj,jk) = 0.25_wp * e1v(ji,jj) * e3v(ji,jj,jk,Kmm) * zpt_v(ji,jj,jk) |
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179 | END_2D |
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180 | ! |
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181 | DO_2D( 1, 0, 1, 0 ) ! horizontal momentum fluxes at T- and F-point |
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182 | zui = ( puu(ji,jj,jk,Kmm) + puu(ji+1,jj ,jk,Kmm) ) |
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183 | zvj = ( pvv(ji,jj,jk,Kmm) + pvv(ji ,jj+1,jk,Kmm) ) |
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184 | ! |
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185 | IF( zui > 0 ) THEN ; zl_u = zlu_uu(ji ,jj,jk,1) |
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186 | ELSE ; zl_u = zlu_uu(ji+1,jj,jk,1) |
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187 | ENDIF |
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188 | IF( zvj > 0 ) THEN ; zl_v = zlv_vv(ji,jj ,jk,1) |
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189 | ELSE ; zl_v = zlv_vv(ji,jj+1,jk,1) |
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190 | ENDIF |
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191 | ! |
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192 | zfu_t(ji+1,jj ,jk) = ( zfu(ji,jj,jk) + zfu(ji+1,jj ,jk) & |
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193 | & - gamma2 * ( zlu_uu(ji,jj,jk,2) + zlu_uu(ji+1,jj ,jk,2) ) ) & |
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194 | & * ( zui - gamma1 * zl_u) |
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195 | zfv_t(ji ,jj+1,jk) = ( zfv(ji,jj,jk) + zfv(ji ,jj+1,jk) & |
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196 | & - gamma2 * ( zlv_vv(ji,jj,jk,2) + zlv_vv(ji ,jj+1,jk,2) ) ) & |
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197 | & * ( zvj - gamma1 * zl_v) |
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198 | ! |
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199 | zfuj = ( zfu(ji,jj,jk) + zfu(ji ,jj+1,jk) ) |
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200 | zfvi = ( zfv(ji,jj,jk) + zfv(ji+1,jj ,jk) ) |
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201 | IF( zfuj > 0 ) THEN ; zl_v = zlv_vu( ji ,jj ,jk,1) |
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202 | ELSE ; zl_v = zlv_vu( ji+1,jj,jk,1) |
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203 | ENDIF |
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204 | IF( zfvi > 0 ) THEN ; zl_u = zlu_uv( ji,jj ,jk,1) |
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205 | ELSE ; zl_u = zlu_uv( ji,jj+1,jk,1) |
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206 | ENDIF |
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207 | ! |
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208 | zfv_f(ji ,jj ,jk) = ( zfvi - gamma2 * ( zlv_vu(ji,jj,jk,2) + zlv_vu(ji+1,jj ,jk,2) ) ) & |
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209 | & * ( puu(ji,jj,jk,Kmm) + puu(ji ,jj+1,jk,Kmm) - gamma1 * zl_u ) |
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210 | zfu_f(ji ,jj ,jk) = ( zfuj - gamma2 * ( zlu_uv(ji,jj,jk,2) + zlu_uv(ji ,jj+1,jk,2) ) ) & |
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211 | & * ( pvv(ji,jj,jk,Kmm) + pvv(ji+1,jj ,jk,Kmm) - gamma1 * zl_v ) |
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212 | END_2D |
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213 | DO_2D( 0, 0, 0, 0 ) ! divergence of horizontal momentum fluxes |
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214 | puu(ji,jj,jk,Krhs) = puu(ji,jj,jk,Krhs) - ( zfu_t(ji+1,jj,jk) - zfu_t(ji,jj ,jk) & |
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215 | & + zfv_f(ji ,jj,jk) - zfv_f(ji,jj-1,jk) ) * r1_e1e2u(ji,jj) & |
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216 | & / e3u(ji,jj,jk,Kmm) |
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217 | pvv(ji,jj,jk,Krhs) = pvv(ji,jj,jk,Krhs) - ( zfu_f(ji,jj ,jk) - zfu_f(ji-1,jj,jk) & |
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218 | & + zfv_t(ji,jj+1,jk) - zfv_t(ji ,jj,jk) ) * r1_e1e2v(ji,jj) & |
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219 | & / e3v(ji,jj,jk,Kmm) |
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220 | END_2D |
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221 | END DO |
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222 | IF( l_trddyn ) THEN ! trends: send trends to trddyn for diagnostic |
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223 | zfu_uw(:,:,:) = puu(:,:,:,Krhs) - zfu_uw(:,:,:) |
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224 | zfv_vw(:,:,:) = pvv(:,:,:,Krhs) - zfv_vw(:,:,:) |
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225 | CALL trd_dyn( zfu_uw, zfv_vw, jpdyn_keg, kt, Kmm ) |
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226 | zfu_t(:,:,:) = puu(:,:,:,Krhs) |
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227 | zfv_t(:,:,:) = pvv(:,:,:,Krhs) |
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228 | ENDIF |
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229 | ! ! ==================== ! |
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230 | ! ! Vertical advection ! |
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231 | ! ! ==================== ! |
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232 | ! |
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233 | ! ! ======================== ! |
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234 | IF( PRESENT( no_zad ) ) THEN ! No vertical advection ! (except if linear free surface) |
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235 | ! ! ======================== ! ------ |
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236 | ! |
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237 | IF( ln_linssh ) THEN ! linear free surface: advection through the surface z=0 |
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238 | DO_2D( 0, 0, 0, 0 ) |
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239 | zzu = 0.5_wp * ( e1e2t(ji,jj) * zpt_w(ji,jj,1) + e1e2t(ji+1,jj) * zpt_w(ji+1,jj,1) ) * puu(ji,jj,1,Kmm) |
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240 | zzv = 0.5_wp * ( e1e2t(ji,jj) * zpt_w(ji,jj,1) + e1e2t(ji,jj+1) * zpt_w(ji,jj+1,1) ) * pvv(ji,jj,1,Kmm) |
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241 | puu(ji,jj,1,Krhs) = puu(ji,jj,1,Krhs) - zzu * r1_e1e2u(ji,jj) & |
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242 | & / e3u(ji,jj,1,Kmm) |
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243 | pvv(ji,jj,1,Krhs) = pvv(ji,jj,1,Krhs) - zzv * r1_e1e2v(ji,jj) & |
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244 | & / e3v(ji,jj,1,Kmm) |
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245 | END_2D |
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246 | ENDIF |
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247 | ! ! =================== ! |
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248 | ELSE ! Vertical advection ! |
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249 | ! ! =================== ! |
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250 | DO_2D( 0, 0, 0, 0 ) ! surface/bottom advective fluxes set to zero |
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251 | zfu_uw(ji,jj,jpk) = 0._wp |
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252 | zfv_vw(ji,jj,jpk) = 0._wp |
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253 | zfu_uw(ji,jj, 1 ) = 0._wp |
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254 | zfv_vw(ji,jj, 1 ) = 0._wp |
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255 | END_2D |
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256 | IF( ln_linssh ) THEN ! constant volume : advection through the surface |
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257 | DO_2D( 0, 0, 0, 0 ) |
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258 | zfu_uw(ji,jj,1) = 0.5_wp * ( e1e2t(ji,jj) * zpt_w(ji,jj,1) + e1e2t(ji+1,jj) * zpt_w(ji+1,jj,1) ) * puu(ji,jj,1,Kmm) |
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259 | zfv_vw(ji,jj,1) = 0.5_wp * ( e1e2t(ji,jj) * zpt_w(ji,jj,1) + e1e2t(ji,jj+1) * zpt_w(ji,jj+1,1) ) * pvv(ji,jj,1,Kmm) |
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260 | END_2D |
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261 | ENDIF |
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262 | DO jk = 2, jpkm1 ! interior fluxes |
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263 | DO_2D( 0, 1, 0, 1 ) |
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264 | zfw(ji,jj,jk) = 0.25_wp * e1e2t(ji,jj) * zpt_w(ji,jj,jk) |
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265 | END_2D |
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266 | DO_2D( 0, 0, 0, 0 ) |
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267 | zfu_uw(ji,jj,jk) = ( zfw(ji,jj,jk)+ zfw(ji+1,jj,jk) ) * ( puu(ji,jj,jk,Kmm) + puu(ji,jj,jk-1,Kmm) ) |
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268 | zfv_vw(ji,jj,jk) = ( zfw(ji,jj,jk)+ zfw(ji,jj+1,jk) ) * ( pvv(ji,jj,jk,Kmm) + pvv(ji,jj,jk-1,Kmm) ) |
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269 | END_2D |
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270 | END DO |
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271 | DO_3D( 0, 0, 0, 0, 1, jpkm1 ) ! divergence of vertical momentum flux divergence |
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272 | puu(ji,jj,jk,Krhs) = puu(ji,jj,jk,Krhs) - ( zfu_uw(ji,jj,jk) - zfu_uw(ji,jj,jk+1) ) * r1_e1e2u(ji,jj) & |
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273 | & / e3u(ji,jj,jk,Kmm) |
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274 | pvv(ji,jj,jk,Krhs) = pvv(ji,jj,jk,Krhs) - ( zfv_vw(ji,jj,jk) - zfv_vw(ji,jj,jk+1) ) * r1_e1e2v(ji,jj) & |
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275 | & / e3v(ji,jj,jk,Kmm) |
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276 | END_3D |
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277 | ! |
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278 | IF( l_trddyn ) THEN ! save the vertical advection trend for diagnostic |
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279 | zfu_t(:,:,:) = puu(:,:,:,Krhs) - zfu_t(:,:,:) |
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280 | zfv_t(:,:,:) = pvv(:,:,:,Krhs) - zfv_t(:,:,:) |
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281 | CALL trd_dyn( zfu_t, zfv_t, jpdyn_zad, kt, Kmm ) |
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282 | ENDIF |
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283 | ! ! Control print |
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284 | IF(sn_cfctl%l_prtctl) CALL prt_ctl( tab3d_1=puu(:,:,:,Krhs), clinfo1=' ubs2 adv - Ua: ', mask1=umask, & |
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285 | & tab3d_2=pvv(:,:,:,Krhs), clinfo2= ' Va: ', mask2=vmask, clinfo3='dyn' ) |
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286 | ! |
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287 | ENDIF |
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288 | ! |
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289 | END SUBROUTINE dyn_adv_ubs |
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290 | |
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291 | !!============================================================================== |
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292 | END MODULE dynadv_ubs |
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