1 | ! |
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2 | ! $Id: diagedyn.F 1999 2014-03-20 09:57:19Z dcugnet $ |
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3 | ! |
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4 | |
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5 | C====================================================================== |
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6 | SUBROUTINE diagedyn(tit,iprt,idiag,idiag2,dtime |
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7 | e , ucov , vcov , ps, p ,pk , teta , q, ql) |
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8 | C====================================================================== |
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9 | C |
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10 | C Purpose: |
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11 | C Calcul la difference d'enthalpie et de masse d'eau entre 2 appels, |
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12 | C et calcul le flux de chaleur et le flux d'eau necessaire a ces |
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13 | C changements. Ces valeurs sont moyennees sur la surface de tout |
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14 | C le globe et sont exprime en W/2 et kg/s/m2 |
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15 | C Outil pour diagnostiquer la conservation de l'energie |
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16 | C et de la masse dans la dynamique. |
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17 | C |
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18 | C |
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19 | c====================================================================== |
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20 | C Arguments: |
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21 | C tit-----imput-A15- Comment added in PRINT (CHARACTER*15) |
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22 | C iprt----input-I- PRINT level ( <=1 : no PRINT) |
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23 | C idiag---input-I- indice dans lequel sera range les nouveaux |
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24 | C bilans d' entalpie et de masse |
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25 | C idiag2--input-I-les nouveaux bilans d'entalpie et de masse |
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26 | C sont compare au bilan de d'enthalpie de masse de |
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27 | C l'indice numero idiag2 |
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28 | C Cas parriculier : si idiag2=0, pas de comparaison, on |
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29 | c sort directement les bilans d'enthalpie et de masse |
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30 | C dtime----input-R- time step (s) |
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31 | C uconv, vconv-input-R- vents covariants (m/s) |
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32 | C ps-------input-R- Surface pressure (Pa) |
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33 | C p--------input-R- pressure at the interfaces |
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34 | C pk-------input-R- pk= (p/Pref)**kappa |
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35 | c teta-----input-R- potential temperature (K) |
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36 | c q--------input-R- vapeur d'eau (kg/kg) |
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37 | c ql-------input-R- liquid watter (kg/kg) |
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38 | c aire-----input-R- mesh surafce (m2) |
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39 | c |
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40 | C the following total value are computed by UNIT of earth surface |
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41 | C |
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42 | C d_h_vcol--output-R- Heat flux (W/m2) define as the Enthalpy |
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43 | c change (J/m2) during one time step (dtime) for the whole |
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44 | C atmosphere (air, watter vapour, liquid and solid) |
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45 | C d_qt------output-R- total water mass flux (kg/m2/s) defined as the |
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46 | C total watter (kg/m2) change during one time step (dtime), |
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47 | C d_qw------output-R- same, for the watter vapour only (kg/m2/s) |
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48 | C d_ql------output-R- same, for the liquid watter only (kg/m2/s) |
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49 | C d_ec------output-R- Cinetic Energy Budget (W/m2) for vertical air column |
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50 | C |
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51 | C |
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52 | C J.L. Dufresne, July 2002 |
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53 | c====================================================================== |
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54 | |
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55 | IMPLICIT NONE |
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56 | C |
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57 | #include "dimensions.h" |
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58 | #include "paramet.h" |
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59 | #include "comgeom.h" |
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60 | #include "iniprint.h" |
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61 | |
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62 | #ifdef CPP_EARTH |
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63 | #include "../phylmd/YOMCST.h" |
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64 | #include "../phylmd/YOETHF.h" |
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65 | #endif |
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66 | C |
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67 | INTEGER imjmp1 |
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68 | PARAMETER( imjmp1=iim*jjp1) |
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69 | c Input variables |
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70 | CHARACTER*15 tit |
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71 | INTEGER iprt,idiag, idiag2 |
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72 | REAL dtime |
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73 | REAL vcov(ip1jm,llm),ucov(ip1jmp1,llm) ! vents covariants |
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74 | REAL ps(ip1jmp1) ! pression au sol |
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75 | REAL p (ip1jmp1,llmp1 ) ! pression aux interfac.des couches |
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76 | REAL pk (ip1jmp1,llm ) ! = (p/Pref)**kappa |
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77 | REAL teta(ip1jmp1,llm) ! temperature potentielle |
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78 | REAL q(ip1jmp1,llm) ! champs eau vapeur |
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79 | REAL ql(ip1jmp1,llm) ! champs eau liquide |
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80 | |
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81 | |
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82 | c Output variables |
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83 | REAL d_h_vcol, d_qt, d_qw, d_ql, d_qs, d_ec |
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84 | C |
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85 | C Local variables |
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86 | c |
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87 | REAL h_vcol_tot, h_dair_tot, h_qw_tot, h_ql_tot |
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88 | . , h_qs_tot, qw_tot, ql_tot, qs_tot , ec_tot |
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89 | c h_vcol_tot-- total enthalpy of vertical air column |
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90 | C (air with watter vapour, liquid and solid) (J/m2) |
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91 | c h_dair_tot-- total enthalpy of dry air (J/m2) |
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92 | c h_qw_tot---- total enthalpy of watter vapour (J/m2) |
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93 | c h_ql_tot---- total enthalpy of liquid watter (J/m2) |
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94 | c h_qs_tot---- total enthalpy of solid watter (J/m2) |
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95 | c qw_tot------ total mass of watter vapour (kg/m2) |
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96 | c ql_tot------ total mass of liquid watter (kg/m2) |
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97 | c qs_tot------ total mass of solid watter (kg/m2) |
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98 | c ec_tot------ total cinetic energy (kg/m2) |
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99 | C |
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100 | REAL masse(ip1jmp1,llm) ! masse d'air |
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101 | REAL vcont(ip1jm,llm),ucont(ip1jmp1,llm) |
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102 | REAL ecin(ip1jmp1,llm) |
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103 | |
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104 | REAL zaire(imjmp1) |
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105 | REAL zps(imjmp1) |
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106 | REAL zairm(imjmp1,llm) |
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107 | REAL zecin(imjmp1,llm) |
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108 | REAL zpaprs(imjmp1,llm) |
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109 | REAL zpk(imjmp1,llm) |
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110 | REAL zt(imjmp1,llm) |
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111 | REAL zh(imjmp1,llm) |
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112 | REAL zqw(imjmp1,llm) |
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113 | REAL zql(imjmp1,llm) |
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114 | REAL zqs(imjmp1,llm) |
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115 | |
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116 | REAL zqw_col(imjmp1) |
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117 | REAL zql_col(imjmp1) |
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118 | REAL zqs_col(imjmp1) |
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119 | REAL zec_col(imjmp1) |
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120 | REAL zh_dair_col(imjmp1) |
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121 | REAL zh_qw_col(imjmp1), zh_ql_col(imjmp1), zh_qs_col(imjmp1) |
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122 | C |
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123 | REAL d_h_dair, d_h_qw, d_h_ql, d_h_qs |
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124 | C |
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125 | REAL airetot, zcpvap, zcwat, zcice |
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126 | C |
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127 | INTEGER i, k, jj, ij , l ,ip1jjm1 |
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128 | C |
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129 | INTEGER ndiag ! max number of diagnostic in parallel |
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130 | PARAMETER (ndiag=10) |
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131 | integer pas(ndiag) |
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132 | save pas |
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133 | data pas/ndiag*0/ |
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134 | C |
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135 | REAL h_vcol_pre(ndiag), h_dair_pre(ndiag), h_qw_pre(ndiag) |
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136 | $ , h_ql_pre(ndiag), h_qs_pre(ndiag), qw_pre(ndiag) |
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137 | $ , ql_pre(ndiag), qs_pre(ndiag) , ec_pre(ndiag) |
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138 | SAVE h_vcol_pre, h_dair_pre, h_qw_pre, h_ql_pre |
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139 | $ , h_qs_pre, qw_pre, ql_pre, qs_pre , ec_pre |
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140 | |
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141 | |
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142 | #ifdef CPP_EARTH |
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143 | c====================================================================== |
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144 | C Compute Kinetic enrgy |
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145 | CALL covcont ( llm , ucov , vcov , ucont, vcont ) |
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146 | CALL enercin ( vcov , ucov , vcont , ucont , ecin ) |
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147 | CALL massdair( p, masse ) |
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148 | c====================================================================== |
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149 | C |
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150 | C |
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151 | print*,'MAIS POURQUOI DONC DIAGEDYN NE MARCHE PAS ?' |
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152 | return |
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153 | C On ne garde les donnees que dans les colonnes i=1,iim |
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154 | DO jj = 1,jjp1 |
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155 | ip1jjm1=iip1*(jj-1) |
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156 | DO ij = 1,iim |
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157 | i=iim*(jj-1)+ij |
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158 | zaire(i)=aire(ij+ip1jjm1) |
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159 | zps(i)=ps(ij+ip1jjm1) |
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160 | ENDDO |
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161 | ENDDO |
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162 | C 3D arrays |
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163 | DO l = 1, llm |
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164 | DO jj = 1,jjp1 |
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165 | ip1jjm1=iip1*(jj-1) |
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166 | DO ij = 1,iim |
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167 | i=iim*(jj-1)+ij |
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168 | zairm(i,l) = masse(ij+ip1jjm1,l) |
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169 | zecin(i,l) = ecin(ij+ip1jjm1,l) |
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170 | zpaprs(i,l) = p(ij+ip1jjm1,l) |
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171 | zpk(i,l) = pk(ij+ip1jjm1,l) |
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172 | zh(i,l) = teta(ij+ip1jjm1,l) |
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173 | zqw(i,l) = q(ij+ip1jjm1,l) |
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174 | zql(i,l) = ql(ij+ip1jjm1,l) |
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175 | zqs(i,l) = 0. |
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176 | ENDDO |
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177 | ENDDO |
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178 | ENDDO |
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179 | C |
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180 | C Reset variables |
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181 | DO i = 1, imjmp1 |
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182 | zqw_col(i)=0. |
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183 | zql_col(i)=0. |
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184 | zqs_col(i)=0. |
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185 | zec_col(i) = 0. |
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186 | zh_dair_col(i) = 0. |
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187 | zh_qw_col(i) = 0. |
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188 | zh_ql_col(i) = 0. |
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189 | zh_qs_col(i) = 0. |
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190 | ENDDO |
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191 | C |
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192 | zcpvap=RCPV |
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193 | zcwat=RCW |
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194 | zcice=RCS |
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195 | C |
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196 | C Compute vertical sum for each atmospheric column |
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197 | C ================================================ |
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198 | DO k = 1, llm |
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199 | DO i = 1, imjmp1 |
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200 | C Watter mass |
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201 | zqw_col(i) = zqw_col(i) + zqw(i,k)*zairm(i,k) |
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202 | zql_col(i) = zql_col(i) + zql(i,k)*zairm(i,k) |
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203 | zqs_col(i) = zqs_col(i) + zqs(i,k)*zairm(i,k) |
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204 | C Cinetic Energy |
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205 | zec_col(i) = zec_col(i) |
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206 | $ +zecin(i,k)*zairm(i,k) |
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207 | C Air enthalpy |
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208 | zt(i,k)= zh(i,k) * zpk(i,k) / RCPD |
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209 | zh_dair_col(i) = zh_dair_col(i) |
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210 | $ + RCPD*(1.-zqw(i,k)-zql(i,k)-zqs(i,k))*zairm(i,k)*zt(i,k) |
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211 | zh_qw_col(i) = zh_qw_col(i) |
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212 | $ + zcpvap*zqw(i,k)*zairm(i,k)*zt(i,k) |
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213 | zh_ql_col(i) = zh_ql_col(i) |
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214 | $ + zcwat*zql(i,k)*zairm(i,k)*zt(i,k) |
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215 | $ - RLVTT*zql(i,k)*zairm(i,k) |
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216 | zh_qs_col(i) = zh_qs_col(i) |
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217 | $ + zcice*zqs(i,k)*zairm(i,k)*zt(i,k) |
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218 | $ - RLSTT*zqs(i,k)*zairm(i,k) |
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219 | |
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220 | END DO |
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221 | ENDDO |
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222 | C |
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223 | C Mean over the planete surface |
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224 | C ============================= |
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225 | qw_tot = 0. |
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226 | ql_tot = 0. |
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227 | qs_tot = 0. |
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228 | ec_tot = 0. |
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229 | h_vcol_tot = 0. |
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230 | h_dair_tot = 0. |
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231 | h_qw_tot = 0. |
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232 | h_ql_tot = 0. |
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233 | h_qs_tot = 0. |
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234 | airetot=0. |
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235 | C |
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236 | do i=1,imjmp1 |
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237 | qw_tot = qw_tot + zqw_col(i) |
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238 | ql_tot = ql_tot + zql_col(i) |
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239 | qs_tot = qs_tot + zqs_col(i) |
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240 | ec_tot = ec_tot + zec_col(i) |
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241 | h_dair_tot = h_dair_tot + zh_dair_col(i) |
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242 | h_qw_tot = h_qw_tot + zh_qw_col(i) |
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243 | h_ql_tot = h_ql_tot + zh_ql_col(i) |
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244 | h_qs_tot = h_qs_tot + zh_qs_col(i) |
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245 | airetot=airetot+zaire(i) |
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246 | END DO |
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247 | C |
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248 | qw_tot = qw_tot/airetot |
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249 | ql_tot = ql_tot/airetot |
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250 | qs_tot = qs_tot/airetot |
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251 | ec_tot = ec_tot/airetot |
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252 | h_dair_tot = h_dair_tot/airetot |
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253 | h_qw_tot = h_qw_tot/airetot |
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254 | h_ql_tot = h_ql_tot/airetot |
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255 | h_qs_tot = h_qs_tot/airetot |
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256 | C |
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257 | h_vcol_tot = h_dair_tot+h_qw_tot+h_ql_tot+h_qs_tot |
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258 | C |
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259 | C Compute the change of the atmospheric state compare to the one |
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260 | C stored in "idiag2", and convert it in flux. THis computation |
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261 | C is performed IF idiag2 /= 0 and IF it is not the first CALL |
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262 | c for "idiag" |
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263 | C =================================== |
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264 | C |
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265 | IF ( (idiag2.gt.0) .and. (pas(idiag2) .ne. 0) ) THEN |
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266 | d_h_vcol = (h_vcol_tot - h_vcol_pre(idiag2) )/dtime |
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267 | d_h_dair = (h_dair_tot- h_dair_pre(idiag2))/dtime |
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268 | d_h_qw = (h_qw_tot - h_qw_pre(idiag2) )/dtime |
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269 | d_h_ql = (h_ql_tot - h_ql_pre(idiag2) )/dtime |
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270 | d_h_qs = (h_qs_tot - h_qs_pre(idiag2) )/dtime |
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271 | d_qw = (qw_tot - qw_pre(idiag2) )/dtime |
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272 | d_ql = (ql_tot - ql_pre(idiag2) )/dtime |
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273 | d_qs = (qs_tot - qs_pre(idiag2) )/dtime |
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274 | d_ec = (ec_tot - ec_pre(idiag2) )/dtime |
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275 | d_qt = d_qw + d_ql + d_qs |
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276 | ELSE |
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277 | d_h_vcol = 0. |
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278 | d_h_dair = 0. |
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279 | d_h_qw = 0. |
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280 | d_h_ql = 0. |
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281 | d_h_qs = 0. |
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282 | d_qw = 0. |
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283 | d_ql = 0. |
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284 | d_qs = 0. |
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285 | d_ec = 0. |
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286 | d_qt = 0. |
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287 | ENDIF |
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288 | C |
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289 | IF (iprt.ge.2) THEN |
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290 | WRITE(6,9000) tit,pas(idiag),d_qt,d_qw,d_ql,d_qs |
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291 | 9000 format('Dyn3d. Watter Mass Budget (kg/m2/s)',A15 |
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292 | $ ,1i6,10(1pE14.6)) |
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293 | WRITE(6,9001) tit,pas(idiag), d_h_vcol |
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294 | 9001 format('Dyn3d. Enthalpy Budget (W/m2) ',A15,1i6,10(F8.2)) |
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295 | WRITE(6,9002) tit,pas(idiag), d_ec |
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296 | 9002 format('Dyn3d. Cinetic Energy Budget (W/m2) ',A15,1i6,10(F8.2)) |
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297 | C WRITE(6,9003) tit,pas(idiag), ec_tot |
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298 | 9003 format('Dyn3d. Cinetic Energy (W/m2) ',A15,1i6,10(E15.6)) |
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299 | WRITE(6,9004) tit,pas(idiag), d_h_vcol+d_ec |
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300 | 9004 format('Dyn3d. Total Energy Budget (W/m2) ',A15,1i6,10(F8.2)) |
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301 | END IF |
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302 | C |
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303 | C Store the new atmospheric state in "idiag" |
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304 | C |
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305 | pas(idiag)=pas(idiag)+1 |
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306 | h_vcol_pre(idiag) = h_vcol_tot |
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307 | h_dair_pre(idiag) = h_dair_tot |
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308 | h_qw_pre(idiag) = h_qw_tot |
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309 | h_ql_pre(idiag) = h_ql_tot |
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310 | h_qs_pre(idiag) = h_qs_tot |
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311 | qw_pre(idiag) = qw_tot |
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312 | ql_pre(idiag) = ql_tot |
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313 | qs_pre(idiag) = qs_tot |
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314 | ec_pre (idiag) = ec_tot |
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315 | C |
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316 | #else |
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317 | write(lunout,*)'diagedyn: Needs Earth physics to function' |
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318 | #endif |
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319 | ! #endif of #ifdef CPP_EARTH |
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320 | RETURN |
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321 | END |
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