1 | subroutine ener_conserv(klon,klev,pdtphys, & |
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2 | & puo,pvo,pto,pqo,pql0,pqs0, & |
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3 | & pun,pvn,ptn,pqn,pqln,pqsn,dtke,masse,exner,d_t_ec) |
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4 | |
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5 | !============================================================= |
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6 | ! Energy conservation |
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7 | ! Based on the TKE equation |
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8 | ! The M2 and N2 terms at the origin of TKE production are |
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9 | ! concerted into heating in the d_t_ec term |
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10 | ! Option 1 is the standard |
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11 | ! 101 is for M2 term only |
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12 | ! 101 for N2 term only |
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13 | ! -1 is a previours treatment for kinetic energy only |
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14 | ! FH (hourdin@lmd.jussieu.fr), 2013/04/25 |
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15 | !============================================================= |
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16 | |
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17 | !============================================================= |
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18 | ! Declarations |
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19 | !============================================================= |
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20 | |
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21 | ! From module |
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22 | USE phys_local_var_mod, ONLY : d_u_vdf,d_v_vdf,d_t_vdf,d_u_ajs,d_v_ajs,d_t_ajs, & |
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23 | & d_u_con,d_v_con,d_t_con,d_t_diss |
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24 | USE phys_local_var_mod, ONLY : d_t_eva,d_t_lsc,d_q_eva,d_q_lsc |
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25 | USE phys_output_var_mod, ONLY : bils_ec,bils_ech,bils_tke,bils_kinetic,bils_enthalp,bils_latent,bils_diss |
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26 | USE add_phys_tend_mod, ONLY : fl_cor_ebil |
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27 | |
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28 | IMPLICIT none |
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29 | #include "YOMCST.h" |
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30 | #include "YOETHF.h" |
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31 | #include "clesphys.h" |
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32 | #include "compbl.h" |
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33 | |
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34 | ! Arguments |
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35 | INTEGER, INTENT(IN) :: klon,klev |
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36 | REAL, INTENT(IN) :: pdtphys |
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37 | REAL, DIMENSION(klon,klev), INTENT(IN) :: puo,pvo,pto,pqo,pql0,pqs0 |
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38 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pun,pvn,ptn,pqn,pqln,pqsn |
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39 | REAL, DIMENSION(klon,klev), INTENT(IN) :: masse,exner |
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40 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: dtke |
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41 | ! |
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42 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_t_ec |
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43 | |
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44 | ! Local |
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45 | integer k,i |
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46 | REAL, DIMENSION(klon,klev+1) :: fluxu,fluxv,fluxt |
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47 | REAL, DIMENSION(klon,klev+1) :: dddu,dddv,dddt |
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48 | REAL, DIMENSION(klon,klev) :: d_u,d_v,d_t,zv,zu,d_t_ech |
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49 | REAL ZRCPD |
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50 | |
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51 | character*80 abort_message |
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52 | character*20 :: modname |
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53 | |
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54 | |
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55 | modname='ener_conser' |
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56 | d_t_ec(:,:)=0. |
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57 | |
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58 | IF (iflag_ener_conserv==-1) THEN |
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59 | !+jld ec_conser |
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60 | DO k = 1, klev |
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61 | DO i = 1, klon |
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62 | IF (fl_cor_ebil .GT. 0) then |
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63 | ZRCPD = RCPD*(1.0+RVTMP2*(pqn(i,k)+pqln(i,k)+pqsn(i,k))) |
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64 | ELSE |
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65 | ZRCPD = RCPD*(1.0+RVTMP2*pqn(i,k)) |
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66 | ENDIF |
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67 | d_t_ec(i,k)=0.5/ZRCPD & |
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68 | & *(puo(i,k)**2+pvo(i,k)**2-pun(i,k)**2-pvn(i,k)**2) |
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69 | ENDDO |
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70 | ENDDO |
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71 | !-jld ec_conser |
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72 | |
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73 | |
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74 | |
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75 | ELSEIF (iflag_ener_conserv>=1) THEN |
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76 | |
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77 | IF (iflag_ener_conserv<=2) THEN |
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78 | ! print*,'ener_conserv pbl=',iflag_pbl |
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79 | IF (iflag_pbl>=20 .AND. iflag_pbl<=27) THEN !d_t_diss accounts for conserv |
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80 | d_t(:,:)=d_t_ajs(:,:) ! d_t_ajs = adjust + thermals |
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81 | d_u(:,:)=d_u_ajs(:,:)+d_u_con(:,:) |
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82 | d_v(:,:)=d_v_ajs(:,:)+d_v_con(:,:) |
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83 | ELSE |
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84 | d_t(:,:)=d_t_vdf(:,:)+d_t_ajs(:,:) ! d_t_ajs = adjust + thermals |
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85 | d_u(:,:)=d_u_vdf(:,:)+d_u_ajs(:,:)+d_u_con(:,:) |
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86 | d_v(:,:)=d_v_vdf(:,:)+d_v_ajs(:,:)+d_v_con(:,:) |
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87 | ENDIF |
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88 | ELSEIF (iflag_ener_conserv==101) THEN |
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89 | d_t(:,:)=0. |
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90 | d_u(:,:)=d_u_vdf(:,:)+d_u_ajs(:,:)+d_u_con(:,:) |
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91 | d_v(:,:)=d_v_vdf(:,:)+d_v_ajs(:,:)+d_v_con(:,:) |
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92 | ELSEIF (iflag_ener_conserv==110) THEN |
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93 | d_t(:,:)=d_t_vdf(:,:)+d_t_ajs(:,:) |
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94 | d_u(:,:)=0. |
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95 | d_v(:,:)=0. |
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96 | ELSE |
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97 | abort_message = 'iflag_ener_conserv non prevu' |
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98 | CALL abort_physic (modname,abort_message,1) |
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99 | ENDIF |
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100 | |
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101 | !---------------------------------------------------------------------------- |
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102 | ! Two options wether we consider time integration in the energy conservation |
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103 | !---------------------------------------------------------------------------- |
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104 | |
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105 | if (iflag_ener_conserv==2) then |
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106 | zu(:,:)=puo(:,:) |
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107 | zv(:,:)=pvo(:,:) |
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108 | else |
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109 | IF (iflag_pbl>=20 .AND. iflag_pbl<=27) THEN |
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110 | zu(:,:)=puo(:,:)+d_u_vdf(:,:)+0.5*d_u(:,:) |
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111 | zv(:,:)=pvo(:,:)+d_v_vdf(:,:)+0.5*d_v(:,:) |
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112 | ELSE |
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113 | zu(:,:)=puo(:,:)+0.5*d_u(:,:) |
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114 | zv(:,:)=pvo(:,:)+0.5*d_v(:,:) |
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115 | ENDIF |
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116 | endif |
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117 | |
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118 | fluxu(:,klev+1)=0. |
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119 | fluxv(:,klev+1)=0. |
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120 | fluxt(:,klev+1)=0. |
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121 | |
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122 | do k=klev,1,-1 |
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123 | fluxu(:,k)=fluxu(:,k+1)+masse(:,k)*d_u(:,k) |
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124 | fluxv(:,k)=fluxv(:,k+1)+masse(:,k)*d_v(:,k) |
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125 | fluxt(:,k)=fluxt(:,k+1)+masse(:,k)*d_t(:,k)/exner(:,k) |
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126 | enddo |
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127 | |
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128 | dddu(:,1)=2*zu(:,1)*fluxu(:,1) |
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129 | dddv(:,1)=2*zv(:,1)*fluxv(:,1) |
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130 | dddt(:,1)=(exner(:,1)-1.)*fluxt(:,1) |
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131 | |
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132 | do k=2,klev |
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133 | dddu(:,k)=(zu(:,k)-zu(:,k-1))*fluxu(:,k) |
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134 | dddv(:,k)=(zv(:,k)-zv(:,k-1))*fluxv(:,k) |
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135 | dddt(:,k)=(exner(:,k)-exner(:,k-1))*fluxt(:,k) |
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136 | enddo |
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137 | dddu(:,klev+1)=0. |
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138 | dddv(:,klev+1)=0. |
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139 | dddt(:,klev+1)=0. |
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140 | |
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141 | do k=1,klev |
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142 | d_t_ech(:,k)=-(rcpd*(dddt(:,k)+dddt(:,k+1)))/(2.*rcpd*masse(:,k)) |
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143 | d_t_ec(:,k)=-(dddu(:,k)+dddu(:,k+1)+dddv(:,k)+dddv(:,k+1))/(2.*rcpd*masse(:,k))+d_t_ech(:,k) |
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144 | enddo |
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145 | |
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146 | ENDIF |
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147 | |
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148 | !================================================================ |
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149 | ! Computation of integrated enthalpie and kinetic energy variation |
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150 | ! FH (hourdin@lmd.jussieu.fr), 2013/04/25 |
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151 | ! bils_ec : energie conservation term |
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152 | ! bils_ech : part of this term linked to temperature |
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153 | ! bils_tke : change of TKE |
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154 | ! bils_diss : dissipation of TKE (when activated) |
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155 | ! bils_kinetic : change of kinetic energie of the column |
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156 | ! bils_enthalp : change of enthalpie |
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157 | ! bils_latent : change of latent heat. Computed between |
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158 | ! after reevaporation (at the beginning of the physics) |
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159 | ! and before large scale condensation (fisrtilp) |
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160 | !================================================================ |
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161 | |
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162 | bils_ec(:)=0. |
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163 | bils_ech(:)=0. |
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164 | bils_tke(:)=0. |
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165 | bils_diss(:)=0. |
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166 | bils_kinetic(:)=0. |
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167 | bils_enthalp(:)=0. |
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168 | bils_latent(:)=0. |
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169 | DO k=1,klev |
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170 | bils_ec(:)=bils_ec(:)-d_t_ec(:,k)*masse(:,k) |
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171 | bils_tke(:)=bils_tke(:)+0.5*(dtke(:,k)+dtke(:,k+1))*masse(:,k) |
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172 | bils_diss(:)=bils_diss(:)-d_t_diss(:,k)*masse(:,k) |
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173 | bils_kinetic(:)=bils_kinetic(:)+masse(:,k)* & |
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174 | & (pun(:,k)*pun(:,k)+pvn(:,k)*pvn(:,k) & |
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175 | & -puo(:,k)*puo(:,k)-pvo(:,k)*pvo(:,k)) |
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176 | bils_enthalp(:)= & |
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177 | & bils_enthalp(:)+masse(:,k)*(ptn(:,k)-pto(:,k)+d_t_ec(:,k)-d_t_eva(:,k)-d_t_lsc(:,k)) |
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178 | ! & bils_enthalp(:)+masse(:,k)*(ptn(:,k)-pto(:,k)+d_t_ec(:,k)) |
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179 | bils_latent(:)=bils_latent(:)+masse(:,k)* & |
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180 | ! & (pqn(:,k)-pqo(:,k)) |
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181 | & (pqn(:,k)-pqo(:,k)-d_q_eva(:,k)-d_q_lsc(:,k)) |
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182 | ENDDO |
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183 | bils_ec(:)=rcpd*bils_ec(:)/pdtphys |
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184 | bils_tke(:)=bils_tke(:)/pdtphys |
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185 | bils_diss(:)=rcpd*bils_diss(:)/pdtphys |
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186 | bils_kinetic(:)= 0.5*bils_kinetic(:)/pdtphys |
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187 | bils_enthalp(:)=rcpd*bils_enthalp(:)/pdtphys |
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188 | bils_latent(:)=rlvtt*bils_latent(:)/pdtphys |
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189 | |
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190 | IF (iflag_ener_conserv>=1) THEN |
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191 | bils_ech(:)=0. |
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192 | DO k=1,klev |
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193 | bils_ech(:)=bils_ech(:)-d_t_ech(:,k)*masse(:,k) |
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194 | ENDDO |
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195 | bils_ech(:)=rcpd*bils_ech(:)/pdtphys |
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196 | ENDIF |
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197 | |
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198 | RETURN |
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199 | |
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200 | END |
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