1 | subroutine evapCH4(ngrid,nlayer,ptimestep,pplev,zzlay,zzlev, & |
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2 | u,v,tsurf,pqCH4, & |
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3 | tankCH4,pdqCH4,dtsurfevap) |
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4 | |
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5 | use radcommon_h, only: gzlat ! Gravity of the planet [m.s-2] |
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6 | use planete_mod, only: z0 ! Surface roughness of the planet [m] |
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7 | use geometry_mod, only: latitude_deg ! Latitude grid of the planet [°] |
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8 | |
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9 | implicit none |
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10 | |
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11 | !==================================================================== |
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12 | ! |
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13 | ! Purpose |
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14 | ! ------- |
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15 | ! Surface flux for methane evaporation. |
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16 | ! The routine calculates the surface flux of methane |
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17 | ! And the latente heat of methane evaporation. |
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18 | ! |
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19 | ! Implicit scheme. |
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20 | ! We start by adding to variables x the physical tendencies already computed. |
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21 | ! We resolve the equation : |
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22 | ! x(t+1) = x(t) + A * (dx/dt) * dt |
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23 | ! |
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24 | ! |
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25 | ! INPUT |
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26 | ! ----- |
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27 | ! ngrid = Number of grid points in the chunk [-] |
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28 | ! nlayer = Number of vertical layers [-] |
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29 | ! ptimestep = Time step [s] |
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30 | ! pplev = Intermediate pressure levels [Pa] |
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31 | ! zzlay = Altitude at the middle of the atmospheric layers (ref : local surf) [m] |
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32 | ! zzlev = Altitude at the atmospheric layer boundaries (ref : local surf) [m] |
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33 | ! u = Zonal component of the wind [m.s-1] |
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34 | ! v = Meridional component of the wind [m.s-1] |
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35 | ! tsurf = Surface temperature [K] |
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36 | ! pqCH4 = Molar fraction of CH4 [mol.mol-1] |
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37 | ! |
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38 | ! |
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39 | ! OUTPUT |
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40 | ! ------ |
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41 | ! tankCH4 = Depth of surface methane tank [m] |
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42 | ! pdqCH4 = Molar fraction tendency of CH4 at the surface [mol.mol-1.s-1] |
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43 | ! dtsurfevap = Evaporation heating rate at the surface [K.s-1] |
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44 | ! |
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45 | ! |
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46 | ! Author |
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47 | ! ------ |
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48 | ! B. de Batz de Trenquelléon (10/2022) |
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49 | ! |
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50 | !==================================================================== |
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51 | |
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52 | |
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53 | !------------------------------------ |
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54 | ! 0. DECLARATIONS |
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55 | !------------------------------------ |
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56 | |
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57 | ! Inputs : |
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58 | !--------- |
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59 | integer, intent(in) :: ngrid |
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60 | integer, intent(in) :: nlayer |
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61 | real, intent(in) :: ptimestep |
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62 | real, intent(in) :: pplev(ngrid,nlayer+1) |
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63 | real, intent(in) :: zzlay(ngrid,nlayer) |
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64 | real, intent(in) :: zzlev(ngrid,nlayer+1) |
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65 | real, intent(in) :: u(ngrid,nlayer) |
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66 | real, intent(in) :: v(ngrid,nlayer) |
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67 | real, intent(in) :: tsurf(ngrid) |
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68 | real, intent(in) :: pqCH4(ngrid,nlayer) |
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69 | |
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70 | ! Outputs : |
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71 | !---------- |
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72 | real, intent(out) :: tankCH4(ngrid) |
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73 | real, intent(out) :: pdqCH4(ngrid) |
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74 | real, intent(out) :: dtsurfevap(ngrid) |
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75 | |
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76 | ! Parameters : |
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77 | !------------- |
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78 | real, parameter :: karman = 0.4 ! Karman constant [-] |
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79 | real, parameter :: humCH4 = 0.4 ! Imposed surface humidity for CH4 [-] |
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80 | |
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81 | real, parameter :: Flnp = 0.10 ! Fraction occupied by lakes (North Pole) |
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82 | real, parameter :: Flsp = 0.01 ! Fraction occupied by lakes (South Pole) |
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83 | real, parameter :: Flml = 1. ! Fraction not infiltrated into the ground (Mid latitudes) |
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84 | |
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85 | real, parameter :: mmolair = 28.e-3 ! Molar mass of air [kg.mol-1] |
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86 | real, parameter :: mmolCH4 = 16.e-3 ! Molar mass of CH4 [kg.mol-1] |
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87 | real, parameter :: rholCH4 = 425. ! Density of liquid CH4 [kg.m-3] |
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88 | |
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89 | real, parameter :: TcCH4 = 190.56 ! Critical point of CH4 [K] |
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90 | real, parameter :: Cplake = 2689992 ! Surface heat capacity for hydrocarbon lakes [J.m-2.K-1] (Tokano 2005) |
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91 | |
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92 | ! Local variables : |
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93 | !------------------ |
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94 | integer :: ig |
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95 | |
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96 | ! Initialisation : |
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97 | real*8 :: Tlake ! Lake temperature [K] |
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98 | real*8 :: rhoair ! Density of air [kg.m-3] |
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99 | real*8 :: ws ! Horizontal wind at the surface [m.s-1] |
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100 | real*8 :: Cd ! Turbulent term [-] |
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101 | real*8 :: qsatCH4 ! Saturation profile of CH4 [mol.mol-1] |
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102 | |
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103 | ! Flux : |
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104 | real*8 :: flux ! Surface flux [kg.m-2.s-1] |
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105 | real*8 :: fluxCH4 ! Surface flux fo CH4 [kg.m-2.s-1.mol.mol-1] |
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106 | |
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107 | ! Variations of CH4 : |
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108 | real*8 :: newpqCH4 ! New molar fraction of CH4 in the first layer [mol.mol-1] |
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109 | real*8 :: dtankCH4 ! Trend of CH4's tank [m] |
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110 | |
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111 | ! Latente heat : |
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112 | real*8 :: ftm, LvCH4 ! Variables for latente heat [-, J.kg-1] |
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113 | |
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114 | |
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115 | !------------------------------------ |
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116 | ! 1. INITIALISATION |
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117 | !------------------------------------ |
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118 | |
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119 | do ig = 1, ngrid ! Main loop on the horizontal grid |
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120 | |
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121 | ! Density of the first layer of the atmosphere [kg.m-3] |
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122 | rhoair = (pplev(ig,1) - pplev(ig,2)) / gzlat(ig,1) / (zzlev(ig,2) - zzlev(ig,1)) |
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123 | |
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124 | ! Horizontal winds at the surface [m.s-1] |
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125 | ws = sqrt(u(ig,1)*u(ig,1) + v(ig,1)*v(ig,1)) * (10. / zzlay(ig,1))**0.2 |
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126 | |
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127 | ! Source of turbulent kinetic energy at the surface [-] (Forget et al. 1999) |
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128 | Cd = (karman / log(1. + zzlay(ig,1)/z0))**2 |
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129 | |
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130 | ! Saturation profile of CH4 [mol.mol-1] (Fray and Schmidt 2009) : |
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131 | Tlake = tsurf(ig) - 7 ! Lakes are 2-7K less than surface. |
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132 | qsatCH4 = (1.0e5 / pplev(ig,1)) * exp(1.051e1 - 1.110e3/Tlake - 4.341e3/Tlake**2 + 1.035e5/Tlake**3 - 7.910e5/Tlake**4) |
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133 | ! CH4 : 0.70 * qsat because of dissolution in N2 |
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134 | qsatCH4 = 0.70 * qsatCH4 |
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135 | |
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136 | ! Flux at the surface [kg.m-2.s-1] : |
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137 | flux = rhoair * Cd * ws |
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138 | |
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139 | ! Surface humidity : |
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140 | qsatCH4 = humCH4 * qsatCH4 |
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141 | |
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142 | ! <North Pole> |
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143 | if (REAL(latitude_deg(ig)) .ge. 70.0) then |
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144 | flux = Flnp * flux |
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145 | ! <South Pole> |
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146 | else if (REAL(latitude_deg(ig)) .le. -70.0) then |
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147 | flux = Flsp * flux |
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148 | ! <Mid Latitudes> |
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149 | else |
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150 | flux = Flml * flux |
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151 | endif |
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152 | |
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153 | ! Empty tank ? |
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154 | if (tankCH4(ig) .le. 1.e-30) then |
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155 | flux = 0.0 |
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156 | tankCH4(ig) = 1.e-30 |
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157 | endif |
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158 | |
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159 | !------------------------------------ |
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160 | ! 2. IMPLICIT SCHEME |
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161 | !------------------------------------ |
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162 | |
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163 | ! Flux of CH4 at the surface [kg.m-2.s-1.mol.mol-1] : |
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164 | fluxCH4 = flux * (qsatCH4 - pqCH4(ig,1)) |
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165 | |
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166 | ! Flux at the surface [kg.m-2.s-1] --> [s-1] : |
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167 | flux = flux / rhoair / (zzlev(ig,2) - zzlev(ig,1)) |
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168 | |
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169 | ! New molar fraction of CH4 in the first layer [mol.mol-1] : |
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170 | newpqCH4 = (pqCH4(ig,1) + flux * ptimestep * qsatCH4) / (1. + flux * ptimestep) |
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171 | |
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172 | ! Trend of CH4's tank [m] |
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173 | dtankCH4 = - (newpqCH4 - pqCH4(ig,1)) * rhoair * (zzlev(ig,2) - zzlev(ig,1)) * mmolCH4 / mmolair / rholCH4 |
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174 | |
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175 | ! New tank depth of CH4 [m] |
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176 | if ((tankCH4(ig) + dtankCH4) .ge. 1.e-30) then |
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177 | tankCH4(ig) = tankCH4(ig) + dtankCH4 |
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178 | else |
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179 | newpqCH4 = tankCH4(ig) / (rhoair * (zzlev(ig,2) - zzlev(ig,1)) * mmolCH4 / mmolair / rholCH4) + pqCH4(ig,1) |
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180 | tankCH4(ig) = 1.e-30 |
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181 | endif |
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182 | |
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183 | ! Trend of CH4's molar fraction in the first layer [mol.mol-1.s-1] |
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184 | pdqCH4(ig) = (newpqCH4 - pqCH4(ig,1)) / ptimestep |
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185 | |
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186 | |
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187 | !------------------------------------ |
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188 | ! 3. LATENTE HEAT |
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189 | !------------------------------------ |
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190 | |
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191 | ftm = (1. - Tlake / TcCH4) |
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192 | if(ftm .le. 1.e-3) then |
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193 | ftm = 1.e-3 |
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194 | endif |
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195 | |
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196 | ! Latente heat of CH4 vaporisation [J.kg-1.mol.mol-1] |
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197 | LvCH4 = 8.314 * TcCH4 * (7.08 * ftm**0.354 + 10.95 * 1.1e-2 * ftm**0.456) / mmolCH4 |
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198 | |
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199 | ! Evaporation heating rate [K.s-1] |
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200 | dtsurfevap(ig) = - (fluxCH4 * LvCH4) / Cplake |
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201 | |
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202 | enddo ! End of main loop on the horizontal grid |
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203 | |
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204 | return |
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205 | |
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206 | end subroutine evapCH4 |
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