1 | MODULE nonoro_gwd_ran_mod |
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2 | |
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3 | IMPLICIT NONE |
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4 | |
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5 | REAL, allocatable, save :: du_nonoro_gwd(:, :) ! Zonal wind tendency due to GWD |
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6 | REAL, allocatable, save :: dv_nonoro_gwd(:, :) ! Meridional wind tendency due to GWD |
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7 | REAL, allocatable, save :: east_gwstress(:, :) ! Eastward stress profile |
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8 | REAL, allocatable, save :: west_gwstress(:, :) ! Westward stress profile |
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9 | !$OMP THREADPRIVATE(du_nonoro_gwd,dv_nonoro_gwd,east_gwstress,west_gwstress) |
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10 | CONTAINS |
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11 | |
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12 | SUBROUTINE nonoro_gwd_ran(ngrid, nlayer, dtime, cpnew, rnew, pp, & |
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13 | zmax_therm, pt, pu, pv, pdt, pdu, pdv, & |
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14 | zustr, zvstr, d_t, d_u, d_v) |
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15 | |
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16 | !-------------------------------------------------------------------------------- |
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17 | ! Parametrization of the momentum flux deposition due to a discrete |
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18 | ! number of gravity waves. |
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19 | ! F. Lott |
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20 | ! Version 14, Gaussian distribution of the source |
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21 | ! LMDz model online version |
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22 | ! ADAPTED FOR VENUS / F. LOTT + S. LEBONNOIS |
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23 | ! Version adapted on 03/04/2013: |
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24 | ! - input flux compensated in the deepest layers |
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25 | ! |
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26 | ! ADAPTED FOR MARS G.GILLI 02/2016 |
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27 | ! Revision with F.Forget 06/2016 Variable EP-flux |
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28 | ! according to |
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29 | ! PBL variation (max |
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30 | ! velocity thermals) |
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31 | ! D.BARDET 01/2020 - reproductibility of |
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32 | ! the launching altitude |
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33 | ! calculation |
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34 | ! - wave characteristic |
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35 | ! calculation using MOD |
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36 | ! - adding east_gwstress |
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37 | ! and west_gwstress variables |
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38 | ! |
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39 | ! ADAPTED FOR GENERIC D.BARDET 01/2020 |
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40 | ! UPDATED J.LIU 12/2021 The rho (density) at the specific |
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41 | ! locations is introduced. The equation |
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42 | ! of EP-flux is corrected by adding the |
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43 | ! term of density at launch (source) |
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44 | ! altitude(level). Bugs in BV,d_u,d_v fixed. |
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45 | !--------------------------------------------------------------------------------- |
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46 | |
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47 | |
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48 | |
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49 | use comcstfi_mod, only: g, pi, r |
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50 | USE ioipsl_getin_p_mod, ONLY : getin_p |
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51 | use vertical_layers_mod, only : presnivs |
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52 | use geometry_mod, only: cell_area |
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53 | #ifdef CPP_XIOS |
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54 | use xios_output_mod, only: send_xios_field |
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55 | #endif |
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56 | implicit none |
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57 | |
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58 | ! 0. DECLARATIONS: |
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59 | |
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60 | ! 0.1 INPUTS |
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61 | |
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62 | INTEGER, intent(in):: ngrid ! number of atmospheric columns |
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63 | INTEGER, intent(in):: nlayer ! number of atmospheric columns |
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64 | REAL, intent(in):: dtime ! Time step of the Physics |
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65 | REAL, intent(in):: zmax_therm(ngrid) ! Altitude of max velocity thermals (m) |
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66 | REAL,INTENT(IN) :: cpnew(ngrid,nlayer)! Cp of the atmosphere |
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67 | REAL,INTENT(IN) :: rnew(ngrid,nlayer) ! R of the atmosphere |
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68 | REAL, intent(in):: pp(ngrid, nlayer) ! Pressure at full levels(Pa) |
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69 | REAL, intent(in):: pt(ngrid, nlayer) ! Temperature at full levels(K) |
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70 | REAL, intent(in):: pu(ngrid, nlayer) ! Zonal wind at full levels(m/s) |
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71 | REAL, intent(in):: pv(ngrid, nlayer) ! Meridional wind at full levels(m/s) |
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72 | REAL, intent(in):: pdt(ngrid, nlayer) ! Tendency on temperature(K/s) |
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73 | REAL, intent(in):: pdu(ngrid, nlayer) ! Tendency on zonal wind(m/s/s) |
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74 | REAL, intent(in):: pdv(ngrid, nlayer) ! Tendency on meridional wind(m/s/s) |
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75 | |
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76 | ! 0.2 OUTPUTS |
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77 | |
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78 | REAL, intent(out):: zustr(ngrid) ! Zonal surface stress |
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79 | REAL, intent(out):: zvstr(ngrid) ! Meridional surface stress |
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80 | REAL, intent(out):: d_t(ngrid, nlayer) ! Tendency on temperature (K/s) due to gravity waves (not used set to zero) |
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81 | REAL, intent(out):: d_u(ngrid, nlayer) ! Tendency on zonal wind (m/s/s) due to gravity waves |
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82 | REAL, intent(out):: d_v(ngrid, nlayer) ! Tendency on meridional wind (m/s/s) due to gravity waves |
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83 | |
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84 | ! 0.3 INTERNAL ARRAYS |
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85 | |
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86 | REAL :: tt(ngrid, nlayer) ! Temperature at full levels |
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87 | REAL :: rho(ngrid, nlayer) ! Mass density at full levels |
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88 | REAL :: uu(ngrid, nlayer) ! Zonal wind at full levels |
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89 | REAL :: vv(ngrid, nlayer) ! Meridional wind at full levels |
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90 | REAL :: bvlow(ngrid) ! initial N at each grid (not used) |
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91 | REAL :: dz ! depth of the GW source if gwd_convective_source=.true. |
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92 | |
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93 | INTEGER ii, jj, ll |
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94 | |
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95 | ! 0.3.0 Time scale of the like cycle of the waves parametrized |
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96 | REAL, parameter:: deltat = 24. * 3600. |
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97 | |
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98 | ! 0.3.1 Gravity waves specifications |
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99 | INTEGER, parameter:: nk = 2 ! number of horizontal wavenumbers |
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100 | INTEGER, parameter:: np = 2 ! directions (eastward and westward) phase speed |
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101 | INTEGER, parameter:: no = 2 ! absolute values of phase speed |
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102 | INTEGER, parameter:: na = 5 ! Number of realizations to get the phase speed |
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103 | INTEGER, parameter:: nw = nk * np *no ! Total numbers of gravity waves |
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104 | INTEGER jk, jp, jo, jw |
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105 | |
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106 | REAL kstar ! Control value to constrain the min horizontal wavenumber by the horizontal resolution |
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107 | REAL, save :: kmax ! Max horizontal wavenumber=N/u, u(=30) zonal wind velocity at launch,lambda min,lambda=2*pi/kmax=62.8 km |
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108 | !$OMP THREADPRIVATE(kmax) |
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109 | !REAL, parameter:: kmax = 4.e-5 ! Max horizontal wavenumber=N/u, u(=70) zonal wind velocity at launch,lambda min,lambda=2*pi/kmax |
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110 | REAL, parameter:: kmin = 2.e-6 ! Min horizontal wavenumber=1/sqrt(DxDy) Dx and Dy horizontal grid,lambda max,lambda=2*pi/kmax=314 km |
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111 | REAL, save :: cmax ! Max horizontal absolute phase velocity=zonal wind at launch |
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112 | !$OMP THREADPRIVATE(cmax) |
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113 | !REAL, parameter:: cmax = 100. ! Test for Saturn: Max horizontal absolute phase velocity |
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114 | !REAL, parameter:: cmax = 70. ! Test for Saturn: Max horizontal absolute phase velocity |
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115 | REAL, parameter:: cmin = 1. ! Min horizontal absolute phase velocity(not used) |
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116 | REAL cpha ! absolute phase velocity frequency |
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117 | REAL zk(nw, ngrid) ! horizontal wavenumber amplitude |
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118 | REAL zp(nw, ngrid) ! horizontal wavenumber angle |
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119 | REAL zo(nw, ngrid) ! absolute frequency |
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120 | |
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121 | REAL intr_freq_m(nw, ngrid) ! Waves Intr. freq. at the 1/2 lev below the full level (previous name: ZOM) |
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122 | REAL intr_freq_p(nw, ngrid) ! Waves Intr. freq. at the 1/2 lev above the full level (previous name: ZOP) |
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123 | REAL wwm(nw, ngrid) ! Wave EP-fluxes at the 1/2 level below the full level |
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124 | REAL wwp(nw, ngrid) ! Wave EP-fluxes at the 1/2 level above the full level |
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125 | REAL u_epflux_p(nw, ngrid) ! Partial zonal flux (=for each wave) at the 1/2 level above the full level (previous name: RUWP) |
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126 | REAL v_epflux_p(nw, ngrid) ! Partial meridional flux (=for each wave) at the 1/2 level above the full level (previous name: RVWP) |
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127 | REAL u_epflux_tot(ngrid, nlayer + 1) ! Total zonal flux (=for all waves (nw)) at the 1/2 level above the full level (3D) (previous name: RUW) |
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128 | REAL v_epflux_tot(ngrid, nlayer + 1) ! Total meridional flux (=for all waves (nw)) at the 1/2 level above the full level (3D) (previous name: RVW) |
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129 | REAL epflux_0(nw, ngrid) ! Fluxes at launching level (previous name: RUW0) |
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130 | REAL, save :: epflux_max ! Max EP flux value at launching altitude (previous name: RUWMAX, tunable) |
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131 | !$OMP THREADPRIVATE(epflux_max) |
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132 | INTEGER launch ! Launching altitude |
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133 | REAL, parameter:: xlaunch = 0.2 ! Control the launching altitude by pressure |
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134 | REAL, parameter:: zmaxth_top = 8000. ! Top of convective layer in m (approx.) |
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135 | |
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136 | REAL prec(ngrid) ! precipitations |
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137 | REAL prmax ! Max value of precipitation |
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138 | |
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139 | ! 0.3.2 Parameters of waves dissipations |
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140 | REAL, save :: sat ! saturation parameter(tunable) |
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141 | !$OMP THREADPRIVATE(sat) |
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142 | REAL, save :: rdiss ! coefficient of dissipation(tunable) |
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143 | !$OMP THREADPRIVATE(rdiss) |
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144 | REAL, parameter:: zoisec = 1.e-10 ! security for intrinsic freguency |
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145 | |
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146 | ! 0.3.3 Background flow at 1/2 levels and vertical coordinate |
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147 | REAL H0bis(ngrid, nlayer) ! characteristic height of the atmosphere |
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148 | REAL, save:: H0 ! characteristic height of the atmosphere |
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149 | !$OMP THREADPRIVATE(H0) |
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150 | !REAL, parameter:: pr = 250 ! Reference pressure [Pa] |
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151 | !REAL, parameter:: tr = 220. ! Reference temperature [K] |
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152 | ! TEST FOR SATURN STRATOSPHERE |
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153 | REAL, parameter:: pr = 110 ! Reference pressure [Pa] |
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154 | REAL, parameter:: tr = 130. ! Reference temperature [K] |
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155 | REAL zh(ngrid, nlayer + 1) ! Log-pressure altitude (constant H0) |
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156 | REAL zhbis(ngrid, nlayer + 1) ! Log-pressure altitude (varying H) |
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157 | REAL uh(ngrid, nlayer + 1) ! Zonal wind at 1/2 levels |
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158 | REAL vh(ngrid, nlayer + 1) ! Meridional wind at 1/2 levels |
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159 | REAL ph(ngrid, nlayer + 1) ! Pressure at 1/2 levels |
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160 | REAL, parameter:: psec = 1.e-12 ! Security to avoid division by 0 pressure(!!IMPORTANT: should be lower than the topmost layer's pressure) |
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161 | REAL bv(ngrid, nlayer + 1) ! Brunt Vaisala freq. at 1/2 levels |
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162 | REAL, parameter:: bvsec = 1.e-6 ! Security to avoid negative BV (!!IMPORTANT: tunable, depends on which Planet) |
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163 | REAL href(nlayer + 1) ! Reference altitude for launching altitude |
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164 | |
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165 | |
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166 | |
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167 | REAL ran_num_1, ran_num_2, ran_num_3 |
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168 | |
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169 | |
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170 | LOGICAL, save :: firstcall = .true. |
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171 | !$OMP THREADPRIVATE(firstcall) |
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172 | LOGICAL, save :: gwd_convective_source = .false. |
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173 | !$OMP THREADPRIVATE(gwd_convective_source) |
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174 | |
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175 | !-------------------------------------------------------------------------------------------------- |
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176 | ! 1. INITIALISATION |
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177 | !-------------------------------------------------------------------------------------------------- |
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178 | IF (firstcall) THEN |
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179 | write(*,*) "nonoro_gwd_ran: FLott non-oro GW scheme is active!" |
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180 | epflux_max = 0.0 ! Default value !! |
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181 | call getin_p("nonoro_gwd_epflux_max", epflux_max) |
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182 | write(*,*) "nonoro_gwd_ran: epflux_max=", epflux_max |
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183 | sat = 1. ! default gravity waves saturation value !! |
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184 | call getin_p("nonoro_gwd_sat", sat) |
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185 | write(*,*) "nonoro_gwd_ran: sat=", sat |
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186 | cmax = 30. ! default gravity waves phase velocity value !! |
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187 | call getin_p("nonoro_gwd_cmax", cmax) |
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188 | write(*,*) "nonoro_gwd_ran: cmax=", cmax |
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189 | rdiss=1 ! default coefficient of dissipation !! |
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190 | call getin_p("nonoro_gwd_rdiss", rdiss) |
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191 | write(*,*) "nonoro_gwd_ran: rdiss=", rdiss |
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192 | kmax = 1.e-4 ! default Max horizontal wavenumber !! |
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193 | call getin_p("nonoro_gwd_kmax", kmax) |
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194 | write(*,*) "nonoro_gwd_ran: kmax=", kmax |
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195 | |
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196 | ! Characteristic vertical scale height |
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197 | H0 = r * tr / g |
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198 | ! Control |
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199 | if (deltat .LT. dtime) THEN |
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200 | call abort_physic("nonoro_gwd_ran","gwd random: deltat lower than dtime!",1) |
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201 | endif |
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202 | if (nlayer .LT. nw) THEN |
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203 | call abort_physic("nonoro_gwd_ran","gwd random: nlayer lower than nw!",1) |
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204 | endif |
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205 | firstcall = .false. |
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206 | ENDIF |
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207 | gwd_convective_source = .false. |
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208 | |
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209 | ! Compute subroutine's current values of temperature and winds |
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210 | tt(:,:) = pt(:,:) + dtime * pdt(:,:) |
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211 | uu(:,:) = pu(:,:) + dtime * pdu(:,:) |
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212 | vv(:,:) = pv(:,:) + dtime * pdv(:,:) |
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213 | ! Compute the real mass density by rho=p/R(T)T |
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214 | DO ll=1,nlayer |
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215 | DO ii=1,ngrid |
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216 | rho(ii,ll) = pp(ii,ll)/(rnew(ii,ll)*tt(ii,ll)) |
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217 | ENDDO |
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218 | ENDDO |
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219 | ! print*,'epflux_max just after firstcall:', epflux_max |
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220 | |
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221 | !-------------------------------------------------------------------------------------------------- |
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222 | ! 2. EVALUATION OF THE BACKGROUND FLOW AT SEMI-LEVELS |
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223 | !-------------------------------------------------------------------------------------------------- |
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224 | ! Pressure and Inv of pressure, temperature at 1/2 level |
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225 | DO ll = 2, nlayer |
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226 | ph(:, ll) = exp((log(pp(:, ll)) + log(pp(:, ll - 1))) / 2.) |
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227 | end DO |
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228 | |
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229 | ph(:, nlayer + 1) = 0. |
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230 | ph(:, 1) = 2. * pp(:, 1) - ph(:, 2) |
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231 | |
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232 | ! Launching altitude for reproductible case |
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233 | DO ll = 2, nlayer |
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234 | href(ll) = exp((log(presnivs(ll)) + log(presnivs(ll - 1))) / 2.) |
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235 | end DO |
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236 | href(nlayer + 1) = 0. |
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237 | href(1) = 2. * presnivs(1) - href(2) |
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238 | |
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239 | launch = 0. |
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240 | DO ll =1, nlayer |
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241 | IF (href (ll) / href(1) > xlaunch) launch = ll |
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242 | end DO |
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243 | |
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244 | ! Log-pressure vertical coordinate |
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245 | !DO ll = 1, nlayer + 1 |
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246 | ! zh(:,ll) = H0 * log(pr / (ph(:,ll) + psec)) |
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247 | !end DO |
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248 | ZH(:,1) = 0. |
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249 | DO LL = 2, nlayer + 1 |
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250 | !ZH(:, LL) = H0 * LOG(PR / (PH(:, LL) + PSEC)) |
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251 | H0bis(:, LL-1) = r * TT(:, LL-1) / g |
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252 | ZH(:, LL) = ZH(:, LL-1) & |
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253 | + H0bis(:, LL-1)*(PH(:, LL-1)-PH(:,LL))/PP(:, LL-1) |
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254 | end DO |
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255 | ZH(:, 1) = H0 * LOG(PR / (PH(:, 1) + PSEC)) |
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256 | |
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257 | ! Winds and Brunt Vaisala frequency |
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258 | DO ll = 2, nlayer |
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259 | uh(:, ll) = 0.5 * (uu(:, ll) + uu(:, ll - 1)) ! Zonal wind |
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260 | vh(:, ll) = 0.5 * (vv(:, ll) + vv(:, ll - 1)) ! Meridional wind |
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261 | |
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262 | BV(:, LL)= G/(0.5 * (TT(:, LL) + TT(:, LL - 1))) & |
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263 | *((TT(:, LL) - TT(:, LL - 1)) / (ZH(:, LL) - ZH(:, LL - 1))+ & |
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264 | G / cpnew(:,LL)) |
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265 | |
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266 | BV(:,LL) =MAX(1.E-12,BV(:,LL)) ! to ensure that BV is positive |
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267 | BV(:,LL) = MAX(BVSEC,SQRT(BV(:,LL))) ! make sure it is not too small |
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268 | end DO |
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269 | |
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270 | bv(:, 1) = bv(:, 2) |
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271 | uh(:, 1) = 0. |
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272 | vh(:, 1) = 0. |
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273 | bv(:, nlayer + 1) = bv(:, nlayer) |
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274 | uh(:, nlayer + 1) = uu(:, nlayer) |
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275 | vh(:, nlayer + 1) = vv(:, nlayer) |
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276 | |
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277 | !----------------------------------------------------------------------------------------------------------------------- |
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278 | ! 3. WAVES CHARACTERISTICS CHOSEN RANDOMLY |
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279 | !----------------------------------------------------------------------------------------------------------------------- |
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280 | ! The mod function of here a weird arguments are used to produce the waves characteristics in a stochastic way |
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281 | DO jw = 1, nw |
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282 | !Angle |
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283 | DO ii = 1, ngrid |
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284 | |
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285 | ran_num_1 = mod(tt(ii, jw) * 10., 1.) |
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286 | ran_num_2 = mod(tt(ii, jw) * 100., 1.) |
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287 | |
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288 | ! Angle (0 or pi so far) |
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289 | zp(jw, ii) = (sign(1., 0.5 - ran_num_1) + 1.) * pi / 2. |
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290 | ! Horizontal wavenumber amplitude |
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291 | ! TN+GG April/June 2020 (rev2381) |
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292 | ! "Individual waves are not supposed to occupy the entire domain, but only a faction of it" Lott+2012 |
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293 | !zk(jw, ii) = kmin + (kmax - kmin) * ran_num_2 |
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294 | kstar = pi / sqrt(cell_area(ii)) |
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295 | zk(jw, ii) = max(kmin,kstar) + (kmax - max(kmin,kstar)) * ran_num_2 |
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296 | |
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297 | ! Horizontal phase speed |
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298 | ! this computation allows to get a gaussian distribution centered on 0 (right ?) |
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299 | ! then cmin is not useful, and it favors small values. |
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300 | cpha = 0. |
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301 | DO jj = 1, na |
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302 | ran_num_3 = mod(tt(ii, jw + 3 * jj)**2, 1.) |
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303 | cpha = cpha + 2. * cmax * & |
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304 | (ran_num_3 - 0.5) * & |
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305 | sqrt(3.) / sqrt(na * 1.) |
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306 | end DO |
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307 | IF (cpha < 0.) THEN |
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308 | cpha = - 1. * cpha |
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309 | zp (jw, ii) = zp(jw, ii) + pi |
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310 | ENDIF |
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311 | ! otherwise, with the computation below, we get a uniform distribution between cmin and cmax. |
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312 | ! ran_num_3 = mod(tt(ii, jw)**2, 1.) |
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313 | ! cpha = cmin + (cmax - cmin) * ran_num_3 |
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314 | |
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315 | ! Intrinsic frequency |
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316 | zo(jw, ii) = cpha * zk(jw, ii) |
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317 | ! Intrinsic frequency is imposed |
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318 | zo(jw, ii) = zo(jw, ii) & |
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319 | + zk(jw, ii) * cos(zp(jw, ii)) * uh(ii, launch) & |
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320 | + zk(jw, ii) * sin(zp(jw, ii)) * vh(ii, launch) |
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321 | ! Momentum flux at launch level |
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322 | epflux_0(jw, ii) = epflux_max & |
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323 | * mod(100. * (uu(ii, jw)**2 + vv(ii, jw)**2), 1.) |
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324 | ENDDO |
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325 | end DO !DO jw = 1, nw |
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326 | |
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327 | ! print*,'epflux_max just after waves charac. ramdon:', epflux_max |
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328 | ! print*,'epflux_0 just after waves charac. ramdon:', epflux_0 |
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329 | |
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330 | !----------------------------------------------------------------------------------------------------------------------- |
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331 | ! 4. COMPUTE THE FLUXES |
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332 | !----------------------------------------------------------------------------------------------------------------------- |
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333 | ! 4.1 Vertical velocity at launching altitude to ensure the correct value to the imposed fluxes. |
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334 | !------------------------------------------------------ |
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335 | DO jw = 1, nw |
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336 | ! Evaluate intrinsic frequency at launching altutide: |
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337 | intr_freq_p(jw, :) = zo(jw, :) & |
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338 | - zk(jw, :) * cos(zp(jw, :)) * uh(:, launch) & |
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339 | - zk(jw, :) * sin(zp(jw, :)) * vh(:, launch) |
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340 | end DO |
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341 | |
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342 | IF (gwd_convective_source) THEN |
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343 | DO jw = 1, nw |
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344 | ! VERSION WITH CONVECTIVE SOURCE ! designed for Earth |
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345 | |
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346 | ! Vertical velocity at launch level, value to ensure the |
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347 | ! imposed mmt flux factor related to the convective forcing: |
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348 | ! precipitations. |
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349 | |
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350 | ! tanh limitation to values above prmax: |
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351 | ! WWP(JW, :) = epflux_0(JW, :) & |
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352 | ! * (r / cpp / H0 * RLVTT * PRMAX * TANH(PREC(:) / PRMAX))**2 |
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353 | ! Here, we neglected the kinetic energy providing of the thermodynamic |
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354 | ! phase change |
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355 | |
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356 | ! |
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357 | |
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358 | ! Factor related to the characteristics of the waves: |
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359 | wwp(jw, :) = wwp(jw, :) * zk(jw, :)**3 / kmin / bvlow(:) & |
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360 | / MAX(ABS(intr_freq_p(jw, :)), zoisec)**3 |
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361 | |
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362 | ! Moderation by the depth of the source (dz here): |
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363 | wwp(jw, :) = wwp(jw, :) & |
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364 | * exp(- bvlow(:)**2 / max(abs(intr_freq_p(jw, :)), zoisec)**2 & |
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365 | * zk(jw, :)**2 * dz**2) |
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366 | |
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367 | ! Put the stress in the right direction: |
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368 | u_epflux_p(jw, :) = intr_freq_p(jw, :) / max(abs(intr_freq_p(jw, :)), zoisec)**2 & |
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369 | * bv(:, launch) * cos(zp(jw, :)) * wwp(jw, :)**2 |
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370 | v_epflux_p(JW, :) = intr_freq_p(jw, :) / max(abs(intr_freq_p(jw, :)), zoisec)**2 & |
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371 | * bv(:, launch) * sin(zp(jw, :)) * wwp(jw, :)**2 |
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372 | end DO |
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373 | ELSE ! VERSION WITHOUT CONVECTIVE SOURCE |
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374 | ! Vertical velocity at launch level, value to ensure the imposed |
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375 | ! mom flux: |
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376 | DO jw = 1, nw |
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377 | ! WW is directly a flux, here, not vertical velocity anymore |
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378 | wwp(jw, :) = epflux_0(JW,:) |
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379 | u_epflux_p(jw, :) = cos(zp(jw, :)) * sign(1., intr_freq_p(jw, :)) * epflux_0(jw, :) |
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380 | v_epflux_p(jw, :) = sin(zp(jw, :)) * sign(1., intr_freq_p(jw, :)) * epflux_0(jw, :) |
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381 | |
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382 | end DO |
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383 | ENDIF |
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384 | |
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385 | ! 4.2 Initial flux at launching altitude |
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386 | !--------------------------------------- |
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387 | u_epflux_tot(:, launch) = 0. |
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388 | v_epflux_tot(:, launch) = 0. |
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389 | DO jw = 1, nw |
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390 | u_epflux_tot(:, launch) = u_epflux_tot(:, launch) + u_epflux_p(jw, :) |
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391 | v_epflux_tot(:, launch) = v_epflux_tot(:, launch) + v_epflux_p(jw, :) |
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392 | end DO |
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393 | |
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394 | ! 4.3 Loop over altitudes, with passage from one level to the next done by: |
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395 | !-------------------------------------------------------------------------- |
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396 | ! i) conserving the EP flux, |
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397 | ! ii) dissipating a little, |
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398 | ! iii) testing critical levels, |
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399 | ! iv) testing the breaking. |
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400 | !-------------------------------------------------------------------------- |
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401 | DO ll = launch, nlayer - 1 |
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402 | ! Warning! all the physics is here (passage from one level to the next |
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403 | DO jw = 1, nw |
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404 | intr_freq_m(jw, :) = intr_freq_p(jw, :) |
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405 | wwm(jw, :) = wwp(jw, :) |
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406 | ! Intrinsic frequency |
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407 | intr_freq_p(jw, :) = zo(jw, :) - zk(jw, :) * cos(zp(jw, :)) * uh(:, ll + 1) & |
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408 | - zk(jw, :) * sin(zp(jw, :)) * vh(:, ll + 1) |
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409 | ! Vertical velocity in flux formulation |
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410 | wwp(jw, :) = min( & |
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411 | ! No breaking (Eq. 6): |
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412 | wwm(jw, :) & |
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413 | ! Dissipation (Eq. 8)! (real rho used here rather than pressure |
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414 | ! parametration because the original code has a bug if the density of |
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415 | ! the planet at the launch altitude not approximate 1): |
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416 | * exp(-rdiss * 2./rho(:, LL + 1) & |
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417 | * ((bv(:, ll + 1) + bv (:, ll)) / 2.)**3 & |
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418 | / max(abs(intr_freq_p(jw, :) + intr_freq_m(jw, :)) / 2., zoisec)**4 & |
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419 | * zk(jw, :)**3 * (zh(:, ll + 1) - zh(:, ll))) , & |
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420 | ! Critical levels (forced to zero if intrinsic frequency |
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421 | ! changes sign) |
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422 | max(0., sign(1., intr_freq_p(jw, :) * intr_freq_m(jw, :))) & |
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423 | ! Saturation (Eq. 12)(rho at launch altitude is imposed by J.Liu. |
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424 | ! Same reason with Eq. 8) |
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425 | * abs(intr_freq_p(jw, :))**3 /(2.0* bv(:, ll + 1)) & |
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426 | * rho(:,launch)*exp(-zh(:, ll + 1) / H0) & |
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427 | * sat**2 * kmin**2 / zk(jw, :)**4) |
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428 | end DO |
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429 | ! END OF W(KB)ARNING |
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430 | |
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431 | ! Evaluate EP-flux from Eq. 7 and give the right orientation to the stress |
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432 | DO jw = 1, nw |
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433 | u_epflux_p(jw, :) = sign(1., intr_freq_p(jw, :)) * cos(zp(jw, :)) * wwp(jw, :) |
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434 | v_epflux_p(jw, :) = sign(1., intr_freq_p(jw, :)) * sin(zp(jw, :)) * wwp(jw, :) |
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435 | end DO |
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436 | |
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437 | u_epflux_tot(:, ll + 1) = 0. |
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438 | v_epflux_tot(:, ll + 1) = 0. |
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439 | DO jw = 1, nw |
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440 | u_epflux_tot(:, ll + 1) = u_epflux_tot(:, ll + 1) + u_epflux_p(jw, :) |
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441 | v_epflux_tot(:, ll + 1) = v_epflux_tot(:, ll + 1) + v_epflux_p(jw, :) |
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442 | east_gwstress(:, ll) = east_gwstress(:, ll) & |
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443 | + max(0., u_epflux_p(jw, ll)) / float(nw) |
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444 | west_gwstress(:, ll) = west_gwstress(:, ll) & |
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445 | + min(0., u_epflux_p(jw, ll)) / float(nw) |
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446 | end DO |
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447 | end DO ! DO LL = LAUNCH, nlayer - 1 |
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448 | |
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449 | ! 5. TENDENCY CALCULATIONS |
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450 | !------------------------- |
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451 | ! 5.1 Flow rectification at the top and in the low layers |
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452 | ! -------------------------------------------------------- |
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453 | ! Warning, this is the total on all GW... |
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454 | |
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455 | u_epflux_tot(:, nlayer + 1) = 0. |
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456 | v_epflux_tot(:, nlayer + 1) = 0. |
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457 | |
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458 | ! Here, big change compared to FLott version: |
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459 | ! We compensate (u_epflux_(:, LAUNCH), ie total emitted upward flux |
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460 | ! over the layers max(1,LAUNCH-3) to LAUNCH-1 |
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461 | DO LL = 1, max(1,LAUNCH-3) |
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462 | u_epflux_tot(:, LL) = 0. |
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463 | v_epflux_tot(:, LL) = 0. |
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464 | end DO |
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465 | DO LL = max(2,LAUNCH-2), LAUNCH-1 |
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466 | u_epflux_tot(:, LL) = u_epflux_tot(:, LL - 1) & |
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467 | + u_epflux_tot(:, LAUNCH) * (PH(:,LL)-PH(:,LL-1)) & |
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468 | / (PH(:,LAUNCH)-PH(:,max(1,LAUNCH-3))) |
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469 | v_epflux_tot(:, LL) = v_epflux_tot(:, LL - 1) & |
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470 | + v_epflux_tot(:, LAUNCH) * (PH(:,LL)-PH(:,LL-1)) & |
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471 | / (PH(:,LAUNCH)-PH(:,max(1,LAUNCH-3))) |
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472 | east_gwstress(:,LL) = east_gwstress(:, LL - 1) & |
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473 | + east_gwstress(:, LAUNCH) * (PH(:,LL)-PH(:,LL-1)) & |
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474 | / (PH(:,LAUNCH)-PH(:,max(1,LAUNCH-3))) |
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475 | west_gwstress(:,LL) = west_gwstress(:, LL - 1) & |
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476 | + west_gwstress(:, LAUNCH) * (PH(:,LL)-PH(:,LL-1)) & |
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477 | / (PH(:,LAUNCH)-PH(:,max(1,LAUNCH-3))) |
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478 | end DO |
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479 | ! This way, the total flux from GW is zero, but there is a net transport |
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480 | ! (upward) that should be compensated by circulation |
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481 | ! and induce additional friction at the surface |
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482 | |
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483 | ! 5.2 AR-1 RECURSIVE FORMULA (13) IN VERSION 4 |
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484 | !--------------------------------------------- |
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485 | DO LL = 1, nlayer |
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486 | !Notice here the d_u and d_v are tendency (i.e. -1/rho*dEP/dz For Mars) but not increment(Venus). |
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487 | d_u(:, LL) = - (u_epflux_tot(:, LL + 1) - u_epflux_tot(:, LL)) & |
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488 | / (rho(:,ll) * (ZH(:, LL + 1) - ZH(:, LL))) |
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489 | d_v(:, LL) = - (v_epflux_tot(:, LL + 1) - v_epflux_tot(:, LL)) & |
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490 | / (rho(:,ll) * (ZH(:, LL + 1) - ZH(:, LL))) |
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491 | ENDDO |
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492 | d_t(:,:) = 0. |
---|
493 | |
---|
494 | ! 5.3 Update tendency of wind with the previous (and saved) values |
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495 | !----------------------------------------------------------------- |
---|
496 | d_u(:,:) = DTIME/DELTAT/REAL(NW) * d_u(:,:) & |
---|
497 | + (1.-DTIME/DELTAT) * du_nonoro_gwd(:,:) |
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498 | d_v(:,:) = DTIME/DELTAT/REAL(NW) * d_v(:,:) & |
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499 | + (1.-DTIME/DELTAT) * dv_nonoro_gwd(:,:) |
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500 | du_nonoro_gwd(:,:) = d_u(:,:) |
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501 | dv_nonoro_gwd(:,:) = d_v(:,:) |
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502 | |
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503 | ! Cosmetic: evaluation of the cumulated stress |
---|
504 | ZUSTR(:) = 0. |
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505 | ZVSTR(:) = 0. |
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506 | DO LL = 1, nlayer |
---|
507 | ZUSTR(:) = ZUSTR(:) + D_U(:, LL) / g * (PH(:, LL + 1) - PH(:, LL)) |
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508 | ZVSTR(:) = ZVSTR(:) + D_V(:, LL) / g * (PH(:, LL + 1) - PH(:, LL)) |
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509 | ENDDO |
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510 | |
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511 | #ifdef CPP_XIOS |
---|
512 | call send_xios_field("du_nonoro", d_u) |
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513 | call send_xios_field("dv_nonoro", d_v) |
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514 | call send_xios_field("east_gwstress", east_gwstress) |
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515 | call send_xios_field("west_gwstress", west_gwstress) |
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516 | #endif |
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517 | |
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518 | END SUBROUTINE nonoro_gwd_ran |
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519 | |
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520 | ! =================================================================== |
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521 | ! Subroutines used to write variables of memory in start files |
---|
522 | ! =================================================================== |
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523 | |
---|
524 | SUBROUTINE ini_nonoro_gwd_ran(ngrid,nlayer) |
---|
525 | |
---|
526 | IMPLICIT NONE |
---|
527 | |
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528 | INTEGER, INTENT (in) :: ngrid ! number of atmospheric columns |
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529 | INTEGER, INTENT (in) :: nlayer ! number of atmospheric layers |
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530 | |
---|
531 | allocate(du_nonoro_gwd(ngrid, nlayer)) |
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532 | allocate(dv_nonoro_gwd(ngrid, nlayer)) |
---|
533 | allocate(east_gwstress(ngrid, nlayer)) |
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534 | allocate(west_gwstress(ngrid, nlayer)) |
---|
535 | |
---|
536 | END SUBROUTINE ini_nonoro_gwd_ran |
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537 | ! ---------------------------------- |
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538 | SUBROUTINE end_nonoro_gwd_ran |
---|
539 | |
---|
540 | IMPLICIT NONE |
---|
541 | |
---|
542 | if (allocated(du_nonoro_gwd)) deallocate(du_nonoro_gwd) |
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543 | if (allocated(dv_nonoro_gwd)) deallocate(dv_nonoro_gwd) |
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544 | if (allocated(east_gwstress)) deallocate(east_gwstress) |
---|
545 | if (allocated(west_gwstress)) deallocate(west_gwstress) |
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546 | |
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547 | END SUBROUTINE end_nonoro_gwd_ran |
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548 | |
---|
549 | END MODULE nonoro_gwd_ran_mod |
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550 | |
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