1 | ! $Id: top_bound.F90 5159 2024-08-02 19:58:25Z abarral $ |
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2 | |
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3 | SUBROUTINE top_bound(vcov, ucov, teta, masse, dt) |
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4 | |
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5 | USE comconst_mod, ONLY: iflag_top_bound, mode_top_bound, & |
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6 | tau_top_bound |
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7 | USE comvert_mod, ONLY: presnivs, preff, scaleheight |
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8 | USE lmdz_iniprint, ONLY: lunout, prt_level |
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9 | USE lmdz_comdissipn, ONLY: tetaudiv, tetaurot, tetah, cdivu, crot, cdivh |
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10 | USE lmdz_comgeom2 |
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11 | |
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12 | USE lmdz_dimensions, ONLY: iim, jjm, llm, ndm |
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13 | USE lmdz_paramet |
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14 | IMPLICIT NONE |
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15 | ! |
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16 | |
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17 | |
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18 | |
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19 | |
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20 | ! .. DISSIPATION LINEAIRE A HAUT NIVEAU, RUN MESO, |
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21 | ! F. LOTT DEC. 2006 |
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22 | ! ( 10/12/06 ) |
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23 | |
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24 | !======================================================================= |
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25 | |
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26 | ! Auteur: F. LOTT |
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27 | ! ------- |
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28 | |
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29 | ! Objet: |
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30 | ! ------ |
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31 | |
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32 | ! Dissipation linéaire (ex top_bound de la physique) |
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33 | |
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34 | !======================================================================= |
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35 | |
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36 | ! top_bound sponge layer model: |
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37 | ! Quenching is modeled as: A(t)=Am+A0*exp(-lambda*t) |
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38 | ! where Am is the zonal average of the field (or zero), and lambda the inverse |
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39 | ! of the characteristic quenching/relaxation time scale |
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40 | ! Thus, assuming Am to be time-independent, field at time t+dt is given by: |
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41 | ! A(t+dt)=A(t)-(A(t)-Am)*(1-exp(-lambda*t)) |
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42 | ! Moreover lambda can be a function of model level (see below), and relaxation |
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43 | ! can be toward the average zonal field or just zero (see below). |
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44 | |
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45 | ! NB: top_bound sponge is only called from leapfrog if ok_strato=.TRUE. |
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46 | |
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47 | ! sponge parameters: (loaded/set in conf_gcm.F ; stored in comconst_mod) |
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48 | ! iflag_top_bound=0 for no sponge |
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49 | ! iflag_top_bound=1 for sponge over 4 topmost layers |
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50 | ! iflag_top_bound=2 for sponge from top to ~1% of top layer pressure |
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51 | ! mode_top_bound=0: no relaxation |
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52 | ! mode_top_bound=1: u and v relax towards 0 |
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53 | ! mode_top_bound=2: u and v relax towards their zonal mean |
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54 | ! mode_top_bound=3: u,v and pot. temp. relax towards their zonal mean |
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55 | ! tau_top_bound : inverse of charactericstic relaxation time scale at |
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56 | ! the topmost layer (Hz) |
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57 | |
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58 | ! Arguments: |
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59 | ! ---------- |
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60 | |
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61 | REAL, INTENT(INOUT) :: ucov(iip1, jjp1, llm) ! covariant zonal wind |
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62 | REAL, INTENT(INOUT) :: vcov(iip1, jjm, llm) ! covariant meridional wind |
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63 | REAL, INTENT(INOUT) :: teta(iip1, jjp1, llm) ! potential temperature |
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64 | REAL, INTENT(IN) :: masse(iip1, jjp1, llm) ! mass of atmosphere |
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65 | REAL, INTENT(IN) :: dt ! time step (s) of sponge model |
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66 | |
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67 | ! Local: |
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68 | ! ------ |
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69 | |
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70 | REAL :: massebx(iip1, jjp1, llm), masseby(iip1, jjm, llm), zm |
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71 | REAL :: uzon(jjp1, llm), vzon(jjm, llm), tzon(jjp1, llm) |
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72 | |
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73 | INTEGER :: i |
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74 | REAL, SAVE :: rdamp(llm) ! quenching coefficient |
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75 | REAL, save :: lambda(llm) ! inverse or quenching time scale (Hz) |
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76 | |
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77 | LOGICAL, SAVE :: first = .TRUE. |
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78 | |
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79 | INTEGER :: j, l |
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80 | |
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81 | IF (iflag_top_bound==0) return |
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82 | |
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83 | IF (first) THEN |
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84 | IF (iflag_top_bound==1) THEN |
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85 | ! sponge quenching over the topmost 4 atmospheric layers |
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86 | lambda(:) = 0. |
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87 | lambda(llm) = tau_top_bound |
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88 | lambda(llm - 1) = tau_top_bound / 2. |
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89 | lambda(llm - 2) = tau_top_bound / 4. |
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90 | lambda(llm - 3) = tau_top_bound / 8. |
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91 | ELSE IF (iflag_top_bound==2) THEN |
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92 | ! sponge quenching over topmost layers down to pressures which are |
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93 | ! higher than 100 times the topmost layer pressure |
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94 | lambda(:) = tau_top_bound & |
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95 | * max(presnivs(llm) / presnivs(:) - 0.01, 0.) |
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96 | endif |
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97 | |
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98 | ! quenching coefficient rdamp(:) |
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99 | ! rdamp(:)=dt*lambda(:) ! Explicit Euler approx. |
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100 | rdamp(:) = 1. - exp(-lambda(:) * dt) |
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101 | |
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102 | WRITE(lunout, *)'TOP_BOUND mode', mode_top_bound |
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103 | WRITE(lunout, *)'Sponge layer coefficients' |
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104 | WRITE(lunout, *)'p (Pa) z(km) tau(s) 1./tau (Hz)' |
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105 | DO l = 1, llm |
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106 | IF (rdamp(l)/=0.) THEN |
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107 | WRITE(lunout, '(6(1pe12.4,1x))') & |
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108 | presnivs(l), log(preff / presnivs(l)) * scaleheight, & |
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109 | 1. / lambda(l), lambda(l) |
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110 | endif |
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111 | enddo |
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112 | first = .FALSE. |
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113 | ENDIF ! of if (first) |
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114 | |
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115 | CALL massbar(masse, massebx, masseby) |
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116 | |
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117 | ! compute zonal average of vcov and u |
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118 | IF (mode_top_bound>=2) THEN |
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119 | DO l = 1, llm |
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120 | DO j = 1, jjm |
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121 | vzon(j, l) = 0. |
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122 | zm = 0. |
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123 | DO i = 1, iim |
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124 | ! NB: we can work using vcov zonal mean rather than v since the |
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125 | ! cv coefficient (which relates the two) only varies with latitudes |
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126 | vzon(j, l) = vzon(j, l) + vcov(i, j, l) * masseby(i, j, l) |
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127 | zm = zm + masseby(i, j, l) |
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128 | enddo |
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129 | vzon(j, l) = vzon(j, l) / zm |
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130 | enddo |
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131 | enddo |
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132 | |
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133 | DO l = 1, llm |
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134 | DO j = 2, jjm ! excluding poles |
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135 | uzon(j, l) = 0. |
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136 | zm = 0. |
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137 | DO i = 1, iim |
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138 | uzon(j, l) = uzon(j, l) + massebx(i, j, l) * ucov(i, j, l) / cu(i, j) |
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139 | zm = zm + massebx(i, j, l) |
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140 | enddo |
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141 | uzon(j, l) = uzon(j, l) / zm |
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142 | enddo |
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143 | enddo |
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144 | else ! ucov and vcov will relax towards 0 |
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145 | vzon(:, :) = 0. |
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146 | uzon(:, :) = 0. |
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147 | ENDIF ! of if (mode_top_bound.ge.2) |
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148 | |
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149 | ! compute zonal average of potential temperature, if necessary |
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150 | IF (mode_top_bound>=3) THEN |
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151 | DO l = 1, llm |
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152 | DO j = 2, jjm ! excluding poles |
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153 | zm = 0. |
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154 | tzon(j, l) = 0. |
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155 | DO i = 1, iim |
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156 | tzon(j, l) = tzon(j, l) + teta(i, j, l) * masse(i, j, l) |
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157 | zm = zm + masse(i, j, l) |
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158 | enddo |
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159 | tzon(j, l) = tzon(j, l) / zm |
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160 | enddo |
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161 | enddo |
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162 | ENDIF ! of if (mode_top_bound.ge.3) |
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163 | |
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164 | IF (mode_top_bound>=1) THEN |
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165 | ! Apply sponge quenching on vcov: |
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166 | DO l = 1, llm |
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167 | DO i = 1, iip1 |
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168 | DO j = 1, jjm |
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169 | vcov(i, j, l) = vcov(i, j, l) & |
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170 | - rdamp(l) * (vcov(i, j, l) - vzon(j, l)) |
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171 | enddo |
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172 | enddo |
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173 | enddo |
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174 | |
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175 | ! Apply sponge quenching on ucov: |
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176 | DO l = 1, llm |
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177 | DO i = 1, iip1 |
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178 | DO j = 2, jjm ! excluding poles |
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179 | ucov(i, j, l) = ucov(i, j, l) & |
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180 | - rdamp(l) * (ucov(i, j, l) - cu(i, j) * uzon(j, l)) |
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181 | enddo |
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182 | enddo |
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183 | enddo |
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184 | ENDIF ! of if (mode_top_bound.ge.1) |
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185 | |
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186 | IF (mode_top_bound>=3) THEN |
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187 | ! Apply sponge quenching on teta: |
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188 | DO l = 1, llm |
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189 | DO i = 1, iip1 |
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190 | DO j = 2, jjm ! excluding poles |
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191 | teta(i, j, l) = teta(i, j, l) & |
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192 | - rdamp(l) * (teta(i, j, l) - tzon(j, l)) |
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193 | enddo |
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194 | enddo |
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195 | enddo |
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196 | ENDIF ! of if (mode_top_bound.ge.3) |
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197 | |
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198 | END SUBROUTINE top_bound |
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