1 | MODULE YOMGEM |
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2 | |
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3 | USE PARKIND1 ,ONLY : JPIM ,JPRB |
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4 | |
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5 | IMPLICIT NONE |
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6 | |
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7 | SAVE |
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8 | |
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9 | ! ------------------------------------------------------------------ |
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10 | |
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11 | !* * Number of grid points |
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12 | |
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13 | ! NGPTOT : Total number of grid columns on a PE |
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14 | ! NGPTOT_CAP : Size of grid points arrays for ALADIN |
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15 | ! NGPTOTMX : Maximum number of grid columns on any of the PEs |
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16 | ! NGPTOTG : Total number of grid columns on the Globe |
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17 | ! NGPTOTL(NPRGPNS,NPRGPEW) : Total number of grid columns on on eacch PE |
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18 | |
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19 | INTEGER(KIND=JPIM) :: NGPTOT |
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20 | INTEGER(KIND=JPIM) :: NGPTOT_CAP |
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21 | INTEGER(KIND=JPIM) :: NGPTOTMX |
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22 | INTEGER(KIND=JPIM) :: NGPTOTG |
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23 | INTEGER(KIND=JPIM),ALLOCATABLE, TARGET :: NGPTOTL(:,:) |
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24 | |
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25 | ! ------------------------------------------------------------------ |
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26 | |
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27 | !* * Defining the transformed sphere |
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28 | |
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29 | ! RMUCEN : MU OF THE POLE OF STRETCHING |
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30 | ! RLOCEN : LONGITUDE OF THE POLE OF STRETCHING |
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31 | ! RSTRET : STRETCHING FACTOR |
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32 | ! NSTTYP : 1 = POLE OF STRETCHING, POLE OF THE COLLOCATION GRID |
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33 | ! AT THE NORTHERN POLE OF THE REAL EARTH. |
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34 | ! 2 = THE POLE OF STRETCHING IS ANYWHERE ON THE REAL EARTH |
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35 | ! AND ON THE EQUATOR OF THE COLLOCATION GRID ON THE MERIDIAN PI. |
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36 | ! THE EQUATOR OF THE COLLOCATION GRID IS TANGENT |
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37 | ! TO A PARALLEL OF THE EARTH. |
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38 | |
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39 | ! NHTYP : 0 = regular grid |
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40 | ! : 1 = number of points proportional to sqrt(1-mu**2) |
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41 | ! : 2 = number of points read on namelist namrgri |
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42 | |
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43 | ! RNLGINC: increment to get non-linear grid |
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44 | |
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45 | ! R4JP inverse de delta(teta) approche a l'ordre 1 |
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46 | ! RC2P1 RSTRET*RSTRET+1. |
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47 | ! RC2M1 RSTRET*RSTRET-1. |
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48 | ! RCOR0 COMPONENT (0,0) OF CORIOLIS |
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49 | ! RCOR1 COMPONENT (0,1) OF CORIOLIS |
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50 | ! RCOR2 COMPONENT (1,1) OF CORIOLIS |
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51 | |
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52 | ! RCOLON(NGPTOT) cosine of longitude on transformed sphere |
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53 | ! RSILON(NGPTOT) sine " " " |
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54 | ! RINDX (NGPTOT) Longitude index |
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55 | ! RINDY (NGPTOT) Latitude index |
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56 | ! RATATH(NGPTOT) RA*TAN(THETA) on real sphere |
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57 | ! RATATX(NGPTOT) Curvature term for LAM (for u eq.) |
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58 | |
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59 | ! NLOEN(NDGSAG:NDGENG) : number of active points on a parallel |
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60 | ! NLOENG(NDGSAG:NDGENG) : global version of NLOEN |
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61 | ! NMEN(NDGSAG:NDGENG) : associated cut-off wave number |
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62 | ! NMENTC(NDGSAG:NDGENG) : same as NMEN but for truncation NTCMAX. |
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63 | ! NMENG(NDGSAG:NDGENG) : global version of NMEN |
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64 | ! NDGLU(0:MAX(NSMAX,NMSMAX)) : number of active points in an hemisphere |
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65 | ! for a given wave number m |
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66 | ! NSTAGP(NGPTOT) : start position of latitude data for boundary fields |
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67 | ! NESTAGP(NGPTOT) : start position of latitude data for boundary fields |
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68 | ! in extension zone (ALADIN). |
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69 | ! NTSTAGP(NGPTOT) : start position of latitude data for boundary fields |
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70 | ! in C+I+E zone (ALADIN). |
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71 | |
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72 | |
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73 | ! REFLRHC : reference length for critical relative humidity (cloud scheme) |
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74 | ! REFLKUO, REFLCAPE, REFLRHC are ONLY to be used in the SETUP |
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75 | ! of TEQK and TEQC and TEQH |
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76 | |
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77 | ! TEQK : ratio between REFLKUO and the model equivalent mesh size |
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78 | ! TEQC : ratio between REFLCAPE and the model equivalent mesh size |
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79 | ! TEQH : ratio between REFLRHC and the model equivalent mesh size |
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80 | |
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81 | ! TEQK, TEQC, TEQH are to be used in the PHYSICS. |
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82 | |
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83 | REAL(KIND=JPRB) :: RMUCEN |
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84 | REAL(KIND=JPRB) :: RLOCEN |
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85 | REAL(KIND=JPRB) :: RSTRET |
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86 | INTEGER(KIND=JPIM) :: NSTTYP |
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87 | INTEGER(KIND=JPIM) :: NHTYP |
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88 | REAL(KIND=JPRB) :: RNLGINC |
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89 | REAL(KIND=JPRB) :: R4JP |
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90 | REAL(KIND=JPRB) :: RC2P1 |
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91 | REAL(KIND=JPRB) :: RC2M1 |
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92 | REAL(KIND=JPRB) :: RCOR0 |
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93 | REAL(KIND=JPRB) :: RCOR1 |
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94 | REAL(KIND=JPRB) :: RCOR2 |
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95 | REAL(KIND=JPRB),ALLOCATABLE:: RCOLON(:) |
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96 | REAL(KIND=JPRB),ALLOCATABLE:: RSILON(:) |
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97 | REAL(KIND=JPRB),ALLOCATABLE:: RINDX(:) |
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98 | REAL(KIND=JPRB),ALLOCATABLE:: RINDY(:) |
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99 | REAL(KIND=JPRB),ALLOCATABLE:: RATATH(:) |
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100 | REAL(KIND=JPRB),ALLOCATABLE:: RATATX(:) |
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101 | INTEGER(KIND=JPIM),ALLOCATABLE:: NLOEN(:) |
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102 | INTEGER(KIND=JPIM),ALLOCATABLE,TARGET :: NLOENG(:) |
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103 | INTEGER(KIND=JPIM),ALLOCATABLE:: NMEN(:) |
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104 | INTEGER(KIND=JPIM),ALLOCATABLE:: NMENTC(:) |
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105 | INTEGER(KIND=JPIM),ALLOCATABLE:: NMENG(:) |
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106 | INTEGER(KIND=JPIM),ALLOCATABLE:: NDGLU(:) |
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107 | INTEGER(KIND=JPIM),ALLOCATABLE:: NSTAGP(:) |
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108 | INTEGER(KIND=JPIM),ALLOCATABLE:: NESTAGP(:) |
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109 | INTEGER(KIND=JPIM),ALLOCATABLE:: NTSTAGP(:) |
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110 | |
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111 | ! ------------------------------------------------------------------ |
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112 | |
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113 | !* * Defining the transformed sphere: physics input |
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114 | |
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115 | REAL(KIND=JPRB) :: REFLRHC |
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116 | REAL(KIND=JPRB) :: TEQH |
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117 | REAL(KIND=JPRB) :: REFLKUO |
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118 | REAL(KIND=JPRB) :: REFLCAPE |
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119 | REAL(KIND=JPRB) :: TEQK |
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120 | REAL(KIND=JPRB) :: TEQC |
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121 | |
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122 | ! ------------------------------------------------------------------ |
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123 | |
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124 | !* * DEFINING THE VERTICAL COORDINATE |
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125 | |
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126 | ! VP00 : REFERENCE PRESSURE FOR DEFINING VERTICAL COORDINATE |
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127 | ! VALH : (0:NFLEVG) |
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128 | ! VBH : (0:NFLEVG) : B of the vertical coordinate |
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129 | ! VETAH : (0:NFLEVG) ; VERTICAL COORDINATE = VALH+VBH |
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130 | ! VETAF : (0:NFLEVG+1) ; VERTICAL COORDINATE ON LAYERS. |
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131 | ! VCUICO: is used to compute denominators of weights |
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132 | ! for semi-Lagrangian vertical interpolations |
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133 | ! applied to full-level variables. |
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134 | ! VCUICOH:is used to compute denominators of weights |
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135 | ! for semi-Lagrangian vertical interpolations |
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136 | ! applied to half-level variables. |
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137 | ! VRLEVX: REAL(NRLEVX) |
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138 | ! NVAUTF: NVAUTF(VRLEVX*eta) is the number of the layer (full level) |
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139 | ! immediately above "eta", and is bounded by 1 and nflevg-1. |
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140 | ! NVAUTH: NVAUTH(VRLEVX*eta) is the number of the interlayer (half level) |
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141 | ! immediately above "eta", and is bounded by 0 and nflevg-1. |
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142 | ! VAH : (0:NFLEVG) ; =VALH*VP00 |
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143 | ! VC : (NFLEVG) ; =VAH(J)*VBH(J-1)-VAH(J-1)*VBH(J) |
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144 | ! VDELB : (NFLEVG) ; =VBH(J)-VBH(J-1) |
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145 | ! VDELA : (NFLEVG) ; =VAH(J)-VAH(J-1) |
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146 | ! VAF : like VAH but at full levels. |
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147 | ! VBF : like VBH but at full levels. |
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148 | ! VRDETAH: 1/[Delta eta] |
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149 | ! TOPPRES: REFERENCE "EVANESCENT" PRESSURE |
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150 | ! TOPPRES allows to solve some calculations of singularities |
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151 | ! when the top pressure of the model is zero (for ex. in |
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152 | ! GPPREF, GPXYB, SUNHBMAT). |
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153 | |
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154 | ! WE HAVE THEN FOR THE HALF LEVEL PRESSURE : VAH + VBH*(SURFACE PRESSURE) |
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155 | |
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156 | ! NOTE THAT THE HALF LEVEL VALUE AT K+.5 IS VXXX(K) |
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157 | ! (THE FULL LEVEL VALUES ARE FROM 1 TO NFLEVG) |
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158 | |
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159 | REAL(KIND=JPRB) :: VP00 |
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160 | REAL(KIND=JPRB),ALLOCATABLE:: VALH(:) |
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161 | REAL(KIND=JPRB),ALLOCATABLE:: VBH(:) |
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162 | REAL(KIND=JPRB),ALLOCATABLE:: VETAH(:) |
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163 | REAL(KIND=JPRB),ALLOCATABLE:: VETAF(:) |
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164 | REAL(KIND=JPRB),ALLOCATABLE:: VCUICO(:,:) |
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165 | REAL(KIND=JPRB),ALLOCATABLE:: VCUICOH(:,:) |
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166 | REAL(KIND=JPRB) :: VRLEVX |
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167 | INTEGER(KIND=JPIM),ALLOCATABLE:: NVAUTF(:) |
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168 | INTEGER(KIND=JPIM),ALLOCATABLE:: NVAUTH(:) |
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169 | REAL(KIND=JPRB),ALLOCATABLE:: VAH(:) |
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170 | REAL(KIND=JPRB),ALLOCATABLE:: VC(:) |
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171 | REAL(KIND=JPRB),ALLOCATABLE:: VDELB(:) |
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172 | REAL(KIND=JPRB),ALLOCATABLE:: VDELA(:) |
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173 | REAL(KIND=JPRB),ALLOCATABLE:: VAF(:) |
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174 | REAL(KIND=JPRB),ALLOCATABLE:: VBF(:) |
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175 | REAL(KIND=JPRB),ALLOCATABLE:: VRDETAH(:) |
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176 | REAL(KIND=JPRB) :: TOPPRES |
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177 | |
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178 | ! ------------------------------------------------------------------ |
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179 | |
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180 | !* * Miscellaneous |
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181 | |
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182 | ! NBEEGP : ??? |
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183 | ! NBNEGP : ??? |
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184 | |
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185 | INTEGER(KIND=JPIM) :: NBEEGP |
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186 | INTEGER(KIND=JPIM) :: NBNEGP |
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187 | |
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188 | ! ------------------------------------------------------------------ |
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189 | END MODULE YOMGEM |
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