1 | module condensation_generic_mod |
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2 | implicit none |
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3 | |
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4 | contains |
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5 | |
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6 | subroutine condensation_generic(ngrid,nlayer,nq,ptimestep, pplev, pplay, & |
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7 | pt, pq, pdt, pdq, pdtlsc, pdqvaplsc, pdqliqlsc, rneb) |
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8 | use ioipsl_getin_p_mod, only: getin_p !-> to get the metallicity |
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9 | use generic_cloud_common_h |
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10 | USE tracer_h |
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11 | USE mod_phys_lmdz_para, only: is_master |
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12 | use generic_tracer_index_mod, only: generic_tracer_index |
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13 | IMPLICIT none |
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14 | |
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15 | !======================================================================= |
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16 | ! |
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17 | ! Purpose |
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18 | ! ------- |
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19 | ! Calculates large-scale condensation of generic tracer "tname". |
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20 | ! By convention, tname ends with the suffix "_vap", as it represents the |
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21 | ! gas phase of the generic tracer |
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22 | ! |
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23 | ! Authors |
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24 | ! ------- |
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25 | ! Adapted from largescale.F90 by Lucas Teinturier & Noé Clément (2022) |
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26 | ! largescale.F90 adapted from the LMDTERRE code by R. Wordsworth (2009) |
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27 | ! Original author Z. X. Li (1993) |
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28 | ! |
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29 | !========================================================================= |
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30 | |
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31 | INTEGER, intent(in) :: ngrid,nlayer,nq |
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32 | |
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33 | ! Arguments |
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34 | REAL, intent(in) :: ptimestep ! intervalle du temps (s) |
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35 | REAL, intent(in) :: pplev(ngrid,nlayer+1) ! pression a inter-couche |
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36 | REAL, intent(in) :: pplay(ngrid,nlayer) ! pression au milieu de couche |
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37 | REAL, intent(in) :: pt(ngrid,nlayer) ! temperature (K) |
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38 | REAL, intent(in) :: pq(ngrid,nlayer,nq) ! tracer mixing ratio (kg/kg) |
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39 | REAL, intent(in) :: pdt(ngrid,nlayer) ! physical temperature tendency (K/s) |
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40 | REAL, intent(in) :: pdq(ngrid,nlayer,nq) ! physical tracer tendency (K/s) |
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41 | ! CHARACTER(*), intent(in) :: tname_vap ! name of the tracer we consider. BY convention, it ends with _vap !!! |
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42 | REAL, intent(out) :: pdtlsc(ngrid,nlayer) ! incrementation de la temperature (K) |
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43 | REAL, intent(out) :: pdqvaplsc(ngrid,nlayer,nq) ! incrementation de la vapeur du traceur |
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44 | REAL, intent(out) :: pdqliqlsc(ngrid,nlayer,nq) ! incrementation du traceur liquide |
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45 | REAL, intent(out) :: rneb(ngrid,nlayer,nq) ! fraction nuageuse |
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46 | |
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47 | ! Options : |
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48 | real, save :: metallicity !metallicity of planet |
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49 | REAL, SAVE :: qvap_deep ! deep mixing ratio of vapor when simulating bottom less planets |
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50 | REAL, SAVE :: qvap_top ! top mixing ratio of vapor when simulating bottom less planets |
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51 | logical, save :: perfect_vap_profile |
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52 | !$OMP THREADPRIVATE(metallicity, qvap_deep, qvap_top, perfect_vap_profile) |
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53 | |
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54 | ! Local variables |
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55 | |
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56 | ! to call only one time the ice/vap pair of a tracer |
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57 | logical call_ice_vap_generic |
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58 | |
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59 | INTEGER i, k , nn, iq |
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60 | INTEGER,PARAMETER :: nitermax=5000 |
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61 | REAL tau ! tau is in seconds and must not be lower than the physical step time. |
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62 | integer k_cold_trap |
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63 | DOUBLE PRECISION,PARAMETER :: alpha=.1,qthreshold=1.d-8 |
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64 | ! JL13: if "careful, T<Tmin in psat water" appears often, you may want to stabilise the model by |
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65 | ! decreasing alpha and increasing nitermax accordingly |
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66 | DOUBLE PRECISION zq(ngrid) |
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67 | DOUBLE PRECISION zcond(ngrid),zcond_iter |
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68 | DOUBLE PRECISION zqs(ngrid) |
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69 | real zt(ngrid),local_p,psat_tmp,dlnpsat_tmp,Lcp,zqs_temp,zdqs |
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70 | real zqs_temp_1, zqs_temp_2, zqs_temp_3 |
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71 | integer igcm_generic_vap, igcm_generic_ice! index of the vap and ice of generic_tracer |
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72 | ! CHARACTER(len=*) :: tname_ice |
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73 | ! evaporation calculations |
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74 | REAL dqevap(ngrid,nlayer),dtevap(ngrid,nlayer) |
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75 | REAL qevap(ngrid,nlayer,nq) |
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76 | REAL tevap(ngrid,nlayer) |
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77 | |
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78 | DOUBLE PRECISION zx_q(ngrid) |
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79 | DOUBLE PRECISION zy_q(ngrid) |
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80 | LOGICAL,SAVE :: firstcall=.true. |
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81 | !$OMP THREADPRIVATE(firstcall) |
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82 | IF (firstcall) THEN |
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83 | write(*,*) "value for metallicity? " |
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84 | metallicity=0.0 ! default value |
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85 | call getin_p("metallicity",metallicity) |
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86 | write(*,*) " metallicity = ",metallicity |
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87 | |
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88 | write(*,*) "Deep generic tracer vapor mixing ratio ? (no effect if negative) " |
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89 | qvap_deep=-1. ! default value |
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90 | call getin_p("qvap_deep",qvap_deep) |
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91 | write(*,*) " qvap_deep = ",qvap_deep |
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92 | |
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93 | write(*,*) "top generic tracer vapor mixing ratio ? (no effect if negative) " |
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94 | qvap_top=-1. ! default value |
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95 | call getin_p("qvap_top",qvap_top) |
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96 | write(*,*) " qvap_top = ",qvap_top |
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97 | |
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98 | write(*,*) " perfect_vap_profile ? " |
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99 | perfect_vap_profile=.false. ! default value |
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100 | call getin_p("perfect_vap_profile",perfect_vap_profile) |
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101 | write(*,*) " perfect_vap_profile = ",perfect_vap_profile |
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102 | |
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103 | firstcall = .false. |
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104 | ENDIF |
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105 | ! Initialisation of outputs and local variables |
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106 | pdtlsc(1:ngrid,1:nlayer) = 0.0 |
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107 | pdqvaplsc(1:ngrid,1:nlayer,1:nq) = 0.0 |
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108 | pdqliqlsc(1:ngrid,1:nlayer,1:nq) = 0.0 |
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109 | dqevap(1:ngrid,1:nlayer)=0.0 |
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110 | dtevap(1:ngrid,1:nlayer)=0.0 |
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111 | qevap(1:ngrid,1:nlayer,1:nq)=0.0 |
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112 | tevap(1:ngrid,1:nlayer)=0.0 |
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113 | rneb(1:ngrid,1:nlayer,1:nq) = 0.0 |
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114 | ! Let's loop on tracers |
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115 | do iq=1,nq |
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116 | |
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117 | call generic_tracer_index(nq,iq,igcm_generic_vap,igcm_generic_ice,call_ice_vap_generic) |
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118 | |
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119 | if(call_ice_vap_generic) then ! to call only one time the ice/vap pair of a tracer |
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120 | m=constants_mass(iq) |
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121 | delta_vapH=constants_delta_vapH(iq) |
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122 | Tref=constants_Tref(iq) |
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123 | Pref=constants_Pref(iq) |
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124 | epsi_generic=constants_epsi_generic(iq) |
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125 | RLVTT_generic=constants_RLVTT_generic(iq) |
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126 | metallicity_coeff=constants_metallicity_coeff(iq) |
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127 | |
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128 | Lcp=RLVTT_generic/cpp ! need to be init here |
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129 | |
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130 | ! Vertical loop (from top to bottom) |
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131 | DO k = nlayer, 1, -1 |
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132 | zt(1:ngrid)=pt(1:ngrid,k)+pdt(1:ngrid,k)*ptimestep |
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133 | |
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134 | ! Computes Psat and the partial condensation |
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135 | DO i = 1, ngrid |
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136 | local_p=pplay(i,k) |
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137 | if(zt(i).le.15.) then |
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138 | print*,'in lsc',i,k,zt(i) |
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139 | ! zt(i)=15. ! check too low temperatures |
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140 | endif |
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141 | zx_q(i) = pq(i,k,igcm_generic_vap)+pdq(i,k,igcm_generic_vap)*ptimestep |
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142 | |
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143 | call Psat_generic(zt(i),local_p,metallicity,psat_tmp,zqs_temp) |
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144 | zy_q(i) = pq(i,k,igcm_generic_ice)+pdq(i,k,igcm_generic_ice)*ptimestep |
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145 | |
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146 | if ((zx_q(i) .le. zqs_temp) .and. (zy_q(i) .eq. 0.)) then |
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147 | ! if we are are not saturated and if there is no ice |
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148 | ! then no change |
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149 | |
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150 | zcond(i) = 0.0d0 |
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151 | |
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152 | else ! if we are saturated : we must evaporate |
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153 | ! if there is ice : we must check if we can condensate |
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154 | |
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155 | ! iterative process to stabilize the scheme when large water amounts JL12 |
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156 | zcond(i) = 0.0d0 |
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157 | Do nn=1,nitermax |
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158 | call Psat_generic(zt(i),local_p,metallicity,psat_tmp,zqs_temp) |
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159 | zqs(i)=zqs_temp |
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160 | call Lcpdqsat_generic(zt(i),local_p,psat_tmp,zqs_temp,zdqs,dlnpsat_tmp) |
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161 | zcond_iter = alpha*(zx_q(i)-zqs(i))/(1.d0+zdqs) |
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162 | !zcond can be negative here |
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163 | zx_q(i) = zx_q(i) - zcond_iter |
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164 | zcond(i) = zcond(i) + zcond_iter |
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165 | zt(i) = zt(i) + zcond_iter*Lcp |
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166 | if (ABS(zcond_iter/alpha/zqs(i)).lt.qthreshold) exit |
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167 | if (nn.eq.nitermax) print*,'itermax in largescale' |
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168 | End do ! niter |
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169 | |
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170 | ! if zcond(i) > 0, zcond(i) is the amount of vapor that we can condensate |
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171 | ! because we are saturated. zcond(i) will not change below |
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172 | ! if zcond(i) < 0, zcond(i) is the amount of ice that we can evaporate. |
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173 | ! We can not evaporate more than the existing ice, |
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174 | ! so the line below is to check how much we can evaporate. |
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175 | ! If there is no ice available, zcond(i) will be 0. (first condidition of "if") |
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176 | |
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177 | zcond(i)=MAX(zcond(i),-(pq(i,k,igcm_generic_ice)+pdq(i,k,igcm_generic_ice)*ptimestep)) |
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178 | |
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179 | endif |
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180 | |
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181 | if (zcond(i) .gt. 0.) then |
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182 | rneb(i,k,iq)=1 |
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183 | else |
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184 | rneb(i,k,iq)=0. |
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185 | endif |
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186 | |
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187 | zcond(i) = zcond(i)/ptimestep |
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188 | ENDDO ! i=1,ngrid |
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189 | |
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190 | !Tendances de t et q |
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191 | pdqvaplsc(1:ngrid,k,igcm_generic_vap) = - zcond(1:ngrid) |
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192 | pdqliqlsc(1:ngrid,k,igcm_generic_ice) = - pdqvaplsc(1:ngrid,k,igcm_generic_vap) |
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193 | pdtlsc(1:ngrid,k) = pdtlsc(1:ngrid,k) + pdqliqlsc(1:ngrid,k,igcm_generic_ice)*Lcp |
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194 | |
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195 | Enddo ! k= nlayer, 1, -1 |
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196 | |
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197 | if ((perfect_vap_profile) .and. (ngrid.eq.1)) then |
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198 | ! perfect_vap_profile is a mode that should a priori only be used in 1D: |
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199 | ! it aims to force the vap profile: |
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200 | ! - below condensation, it is forced to qvap_deep |
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201 | ! - at condensation levels, it is forced to 99% of sat |
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202 | ! - above the cold trap, it is forced to the value allowed by the cold trap |
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203 | tau=3*24*3600 |
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204 | |
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205 | k_cold_trap = 2 |
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206 | do k=2,nlayer-1 |
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207 | |
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208 | zt(1)=pt(1,k-1)+pdt(1,k-1)*ptimestep |
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209 | call Psat_generic(zt(1),pplay(1,k-1),metallicity,psat_tmp,zqs_temp_1) |
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210 | zt(1)=pt(1,k)+pdt(1,k)*ptimestep |
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211 | call Psat_generic(zt(1),pplay(1,k),metallicity,psat_tmp,zqs_temp_2) |
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212 | zt(1)=pt(1,k+1)+pdt(1,k+1)*ptimestep |
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213 | call Psat_generic(zt(1),pplay(1,k+1),metallicity,psat_tmp,zqs_temp_3) |
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214 | |
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215 | if ((zqs_temp_1 .gt. zqs_temp_2) .and. (zqs_temp_3 .gt. zqs_temp_2)) then |
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216 | k_cold_trap = k |
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217 | exit |
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218 | endif |
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219 | enddo |
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220 | if (k_cold_trap .lt. nlayer) then |
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221 | do k=k_cold_trap+1,nlayer |
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222 | pdqvaplsc(1,k,igcm_generic_vap) = (pq(1,k_cold_trap,igcm_generic_vap) - pq(1,k,igcm_generic_vap))/tau - pdq(1,k,igcm_generic_vap) |
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223 | enddo |
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224 | endif |
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225 | |
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226 | do k=1,k_cold_trap |
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227 | zt(1)=pt(1,k)+pdt(1,k)*ptimestep |
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228 | call Psat_generic(zt(1),pplay(1,k),metallicity,psat_tmp,zqs_temp) |
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229 | if (zqs_temp .gt. qvap_deep) then |
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230 | pdqvaplsc(1,k,igcm_generic_vap) = (qvap_deep - pq(1,k,igcm_generic_vap))/tau - pdq(1,k,igcm_generic_vap) |
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231 | endif |
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232 | if (zqs_temp .lt. qvap_deep) then |
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233 | pdqvaplsc(1,k,igcm_generic_vap) = (0.99*zqs_temp - pq(1,k,igcm_generic_vap))/tau - pdq(1,k,igcm_generic_vap) |
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234 | endif |
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235 | enddo |
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236 | |
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237 | pdqliqlsc(1:ngrid,:,igcm_generic_ice) = 0. |
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238 | pdtlsc(1:ngrid,:) = 0. |
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239 | endif |
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240 | |
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241 | if (qvap_deep >= 0.) then |
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242 | if (ngrid.eq.1) then ! if 1D |
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243 | tau=3*24*3600 ! tau must not be lower than the physical step time. In 1D time step is very long |
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244 | else |
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245 | tau=3600 ! for 3D |
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246 | endif |
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247 | !brings lower generic vapor ratio to a fixed value. |
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248 | ! tau is in seconds and must not be lower than the physical step time. |
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249 | pdqvaplsc(1:ngrid,1,igcm_generic_vap) = (qvap_deep - pq(1:ngrid,1,igcm_generic_vap))/tau - pdq(1:ngrid,1,igcm_generic_vap) |
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250 | endif |
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251 | if (qvap_top >= 0.) then |
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252 | if (ngrid.eq.1) then ! if 1D |
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253 | tau=3*24*3600 ! tau must not be lower than the physical step time. In 1D time step is very long |
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254 | else |
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255 | tau=3600 ! for 3D |
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256 | endif |
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257 | !brings lower generic vapor ratio to a fixed value. |
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258 | ! tau is in seconds and must not be lower than the physical step time. |
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259 | pdqvaplsc(1:ngrid,nlayer,igcm_generic_vap) = (qvap_top - pq(1:ngrid,nlayer,igcm_generic_vap))/tau - pdq(1:ngrid,nlayer,igcm_generic_vap) |
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260 | endif |
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261 | endif !if(call_ice_vap_generic) |
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262 | enddo ! iq=1,nq |
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263 | |
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264 | end subroutine condensation_generic |
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265 | end module condensation_generic_mod |
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