| [524] | 1 | ! |
|---|
| 2 | ! $Header$ |
|---|
| 3 | ! |
|---|
| 4 | SUBROUTINE diagphy(airephy,tit,iprt |
|---|
| 5 | $ , tops, topl, sols, soll, sens |
|---|
| 6 | $ , evap, rain_fall, snow_fall, ts |
|---|
| 7 | $ , d_etp_tot, d_qt_tot, d_ec_tot |
|---|
| 8 | $ , fs_bound, fq_bound) |
|---|
| 9 | C====================================================================== |
|---|
| 10 | C |
|---|
| 11 | C Purpose: |
|---|
| 12 | C Compute the thermal flux and the watter mass flux at the atmosphere |
|---|
| 13 | c boundaries. Print them and also the atmospheric enthalpy change and |
|---|
| 14 | C the atmospheric mass change. |
|---|
| 15 | C |
|---|
| 16 | C Arguments: |
|---|
| 17 | C airephy-------input-R- grid area |
|---|
| 18 | C tit---------input-A15- Comment to be added in PRINT (CHARACTER*15) |
|---|
| 19 | C iprt--------input-I- PRINT level ( <=0 : no PRINT) |
|---|
| 20 | C tops(klon)--input-R- SW rad. at TOA (W/m2), positive up. |
|---|
| 21 | C topl(klon)--input-R- LW rad. at TOA (W/m2), positive down |
|---|
| 22 | C sols(klon)--input-R- Net SW flux above surface (W/m2), positive up |
|---|
| 23 | C (i.e. -1 * flux absorbed by the surface) |
|---|
| 24 | C soll(klon)--input-R- Net LW flux above surface (W/m2), positive up |
|---|
| 25 | C (i.e. flux emited - flux absorbed by the surface) |
|---|
| 26 | C sens(klon)--input-R- Sensible Flux at surface (W/m2), positive down |
|---|
| 27 | C evap(klon)--input-R- Evaporation + sublimation watter vapour mass flux |
|---|
| 28 | C (kg/m2/s), positive up |
|---|
| 29 | C rain_fall(klon) |
|---|
| 30 | C --input-R- Liquid watter mass flux (kg/m2/s), positive down |
|---|
| 31 | C snow_fall(klon) |
|---|
| 32 | C --input-R- Solid watter mass flux (kg/m2/s), positive down |
|---|
| 33 | C ts(klon)----input-R- Surface temperature (K) |
|---|
| 34 | C d_etp_tot---input-R- Heat flux equivalent to atmospheric enthalpy |
|---|
| 35 | C change (W/m2) |
|---|
| 36 | C d_qt_tot----input-R- Mass flux equivalent to atmospheric watter mass |
|---|
| 37 | C change (kg/m2/s) |
|---|
| 38 | C d_ec_tot----input-R- Flux equivalent to atmospheric cinetic energy |
|---|
| 39 | C change (W/m2) |
|---|
| 40 | C |
|---|
| 41 | C fs_bound---output-R- Thermal flux at the atmosphere boundaries (W/m2) |
|---|
| 42 | C fq_bound---output-R- Watter mass flux at the atmosphere boundaries (kg/m2/s) |
|---|
| 43 | C |
|---|
| 44 | C J.L. Dufresne, July 2002 |
|---|
| 45 | C====================================================================== |
|---|
| 46 | C |
|---|
| 47 | implicit none |
|---|
| 48 | |
|---|
| 49 | #include "dimensions.h" |
|---|
| 50 | #include "dimphy.h" |
|---|
| 51 | #include "YOMCST.h" |
|---|
| 52 | #include "YOETHF.h" |
|---|
| 53 | C |
|---|
| 54 | C Input variables |
|---|
| 55 | real airephy(klon) |
|---|
| 56 | CHARACTER*15 tit |
|---|
| 57 | INTEGER iprt |
|---|
| 58 | real tops(klon),topl(klon),sols(klon),soll(klon) |
|---|
| 59 | real sens(klon),evap(klon),rain_fall(klon),snow_fall(klon) |
|---|
| 60 | REAL ts(klon) |
|---|
| 61 | REAL d_etp_tot, d_qt_tot, d_ec_tot |
|---|
| 62 | c Output variables |
|---|
| 63 | REAL fs_bound, fq_bound |
|---|
| 64 | C |
|---|
| 65 | C Local variables |
|---|
| 66 | real stops,stopl,ssols,ssoll |
|---|
| 67 | real ssens,sfront,slat |
|---|
| 68 | real airetot, zcpvap, zcwat, zcice |
|---|
| 69 | REAL rain_fall_tot, snow_fall_tot, evap_tot |
|---|
| 70 | C |
|---|
| 71 | integer i |
|---|
| 72 | C |
|---|
| 73 | integer pas |
|---|
| 74 | save pas |
|---|
| 75 | data pas/0/ |
|---|
| [704] | 76 | c$OMP THREADPRIVATE(pas) |
|---|
| [524] | 77 | C |
|---|
| 78 | pas=pas+1 |
|---|
| 79 | stops=0. |
|---|
| 80 | stopl=0. |
|---|
| 81 | ssols=0. |
|---|
| 82 | ssoll=0. |
|---|
| 83 | ssens=0. |
|---|
| 84 | sfront = 0. |
|---|
| 85 | evap_tot = 0. |
|---|
| 86 | rain_fall_tot = 0. |
|---|
| 87 | snow_fall_tot = 0. |
|---|
| 88 | airetot=0. |
|---|
| 89 | C |
|---|
| 90 | C Pour les chaleur specifiques de la vapeur d'eau, de l'eau et de |
|---|
| 91 | C la glace, on travaille par difference a la chaleur specifique de l' |
|---|
| 92 | c air sec. En effet, comme on travaille a niveau de pression donne, |
|---|
| 93 | C toute variation de la masse d'un constituant est totalement |
|---|
| 94 | c compense par une variation de masse d'air. |
|---|
| 95 | C |
|---|
| 96 | zcpvap=RCPV-RCPD |
|---|
| 97 | zcwat=RCW-RCPD |
|---|
| 98 | zcice=RCS-RCPD |
|---|
| 99 | C |
|---|
| 100 | do i=1,klon |
|---|
| 101 | stops=stops+tops(i)*airephy(i) |
|---|
| 102 | stopl=stopl+topl(i)*airephy(i) |
|---|
| 103 | ssols=ssols+sols(i)*airephy(i) |
|---|
| 104 | ssoll=ssoll+soll(i)*airephy(i) |
|---|
| 105 | ssens=ssens+sens(i)*airephy(i) |
|---|
| 106 | sfront = sfront |
|---|
| 107 | $ + ( evap(i)*zcpvap-rain_fall(i)*zcwat-snow_fall(i)*zcice |
|---|
| 108 | $ ) *ts(i) *airephy(i) |
|---|
| 109 | evap_tot = evap_tot + evap(i)*airephy(i) |
|---|
| 110 | rain_fall_tot = rain_fall_tot + rain_fall(i)*airephy(i) |
|---|
| 111 | snow_fall_tot = snow_fall_tot + snow_fall(i)*airephy(i) |
|---|
| 112 | airetot=airetot+airephy(i) |
|---|
| 113 | enddo |
|---|
| 114 | stops=stops/airetot |
|---|
| 115 | stopl=stopl/airetot |
|---|
| 116 | ssols=ssols/airetot |
|---|
| 117 | ssoll=ssoll/airetot |
|---|
| 118 | ssens=ssens/airetot |
|---|
| 119 | sfront = sfront/airetot |
|---|
| 120 | evap_tot = evap_tot /airetot |
|---|
| 121 | rain_fall_tot = rain_fall_tot/airetot |
|---|
| 122 | snow_fall_tot = snow_fall_tot/airetot |
|---|
| 123 | C |
|---|
| 124 | slat = RLVTT * rain_fall_tot + RLSTT * snow_fall_tot |
|---|
| 125 | C Heat flux at atm. boundaries |
|---|
| 126 | fs_bound = stops-stopl - (ssols+ssoll)+ssens+sfront |
|---|
| 127 | $ + slat |
|---|
| 128 | C Watter flux at atm. boundaries |
|---|
| 129 | fq_bound = evap_tot - rain_fall_tot -snow_fall_tot |
|---|
| 130 | C |
|---|
| 131 | IF (iprt.ge.1) write(6,6666) |
|---|
| 132 | $ tit, pas, fs_bound, d_etp_tot, fq_bound, d_qt_tot |
|---|
| 133 | C |
|---|
| 134 | IF (iprt.ge.1) write(6,6668) |
|---|
| 135 | $ tit, pas, d_etp_tot+d_ec_tot-fs_bound, d_qt_tot-fq_bound |
|---|
| 136 | C |
|---|
| 137 | IF (iprt.ge.2) write(6,6667) |
|---|
| 138 | $ tit, pas, stops,stopl,ssols,ssoll,ssens,slat,evap_tot |
|---|
| 139 | $ ,rain_fall_tot+snow_fall_tot |
|---|
| 140 | |
|---|
| 141 | return |
|---|
| 142 | |
|---|
| 143 | 6666 format('Phys. Flux Budget ',a15,1i6,2f8.2,2(1pE13.5)) |
|---|
| 144 | 6667 format('Phys. Boundary Flux ',a15,1i6,6f8.2,2(1pE13.5)) |
|---|
| 145 | 6668 format('Phys. Total Budget ',a15,1i6,f8.2,2(1pE13.5)) |
|---|
| 146 | |
|---|
| 147 | end |
|---|
| 148 | |
|---|
| 149 | C====================================================================== |
|---|
| 150 | SUBROUTINE diagetpq(airephy,tit,iprt,idiag,idiag2,dtime |
|---|
| 151 | e ,t,q,ql,qs,u,v,paprs,pplay |
|---|
| 152 | s , d_h_vcol, d_qt, d_qw, d_ql, d_qs, d_ec) |
|---|
| 153 | C====================================================================== |
|---|
| 154 | C |
|---|
| 155 | C Purpose: |
|---|
| 156 | C Calcul la difference d'enthalpie et de masse d'eau entre 2 appels, |
|---|
| 157 | C et calcul le flux de chaleur et le flux d'eau necessaire a ces |
|---|
| 158 | C changements. Ces valeurs sont moyennees sur la surface de tout |
|---|
| 159 | C le globe et sont exprime en W/2 et kg/s/m2 |
|---|
| 160 | C Outil pour diagnostiquer la conservation de l'energie |
|---|
| 161 | C et de la masse dans la physique. Suppose que les niveau de |
|---|
| 162 | c pression entre couche ne varie pas entre 2 appels. |
|---|
| 163 | C |
|---|
| 164 | C Plusieurs de ces diagnostics peuvent etre fait en parallele: les |
|---|
| 165 | c bilans sont sauvegardes dans des tableaux indices. On parlera |
|---|
| 166 | C "d'indice de diagnostic" |
|---|
| 167 | c |
|---|
| 168 | C |
|---|
| 169 | c====================================================================== |
|---|
| 170 | C Arguments: |
|---|
| 171 | C airephy-------input-R- grid area |
|---|
| 172 | C tit-----imput-A15- Comment added in PRINT (CHARACTER*15) |
|---|
| 173 | C iprt----input-I- PRINT level ( <=1 : no PRINT) |
|---|
| 174 | C idiag---input-I- indice dans lequel sera range les nouveaux |
|---|
| 175 | C bilans d' entalpie et de masse |
|---|
| 176 | C idiag2--input-I-les nouveaux bilans d'entalpie et de masse |
|---|
| 177 | C sont compare au bilan de d'enthalpie de masse de |
|---|
| 178 | C l'indice numero idiag2 |
|---|
| 179 | C Cas parriculier : si idiag2=0, pas de comparaison, on |
|---|
| 180 | c sort directement les bilans d'enthalpie et de masse |
|---|
| 181 | C dtime----input-R- time step (s) |
|---|
| 182 | c t--------input-R- temperature (K) |
|---|
| 183 | c q--------input-R- vapeur d'eau (kg/kg) |
|---|
| 184 | c ql-------input-R- liquid watter (kg/kg) |
|---|
| 185 | c qs-------input-R- solid watter (kg/kg) |
|---|
| 186 | c u--------input-R- vitesse u |
|---|
| 187 | c v--------input-R- vitesse v |
|---|
| 188 | c paprs----input-R- pression a intercouche (Pa) |
|---|
| 189 | c pplay----input-R- pression au milieu de couche (Pa) |
|---|
| 190 | c |
|---|
| 191 | C the following total value are computed by UNIT of earth surface |
|---|
| 192 | C |
|---|
| 193 | C d_h_vcol--output-R- Heat flux (W/m2) define as the Enthalpy |
|---|
| 194 | c change (J/m2) during one time step (dtime) for the whole |
|---|
| 195 | C atmosphere (air, watter vapour, liquid and solid) |
|---|
| 196 | C d_qt------output-R- total water mass flux (kg/m2/s) defined as the |
|---|
| 197 | C total watter (kg/m2) change during one time step (dtime), |
|---|
| 198 | C d_qw------output-R- same, for the watter vapour only (kg/m2/s) |
|---|
| 199 | C d_ql------output-R- same, for the liquid watter only (kg/m2/s) |
|---|
| 200 | C d_qs------output-R- same, for the solid watter only (kg/m2/s) |
|---|
| 201 | C d_ec------output-R- Cinetic Energy Budget (W/m2) for vertical air column |
|---|
| 202 | C |
|---|
| 203 | C other (COMMON...) |
|---|
| 204 | C RCPD, RCPV, .... |
|---|
| 205 | C |
|---|
| 206 | C J.L. Dufresne, July 2002 |
|---|
| 207 | c====================================================================== |
|---|
| 208 | |
|---|
| 209 | IMPLICIT NONE |
|---|
| 210 | C |
|---|
| 211 | #include "dimensions.h" |
|---|
| 212 | #include "dimphy.h" |
|---|
| 213 | #include "YOMCST.h" |
|---|
| 214 | #include "YOETHF.h" |
|---|
| 215 | C |
|---|
| 216 | c Input variables |
|---|
| 217 | real airephy(klon) |
|---|
| 218 | CHARACTER*15 tit |
|---|
| 219 | INTEGER iprt,idiag, idiag2 |
|---|
| 220 | REAL dtime |
|---|
| 221 | REAL t(klon,klev), q(klon,klev), ql(klon,klev), qs(klon,klev) |
|---|
| 222 | REAL u(klon,klev), v(klon,klev) |
|---|
| 223 | REAL paprs(klon,klev+1), pplay(klon,klev) |
|---|
| 224 | c Output variables |
|---|
| 225 | REAL d_h_vcol, d_qt, d_qw, d_ql, d_qs, d_ec |
|---|
| 226 | C |
|---|
| 227 | C Local variables |
|---|
| 228 | c |
|---|
| 229 | REAL h_vcol_tot, h_dair_tot, h_qw_tot, h_ql_tot |
|---|
| 230 | . , h_qs_tot, qw_tot, ql_tot, qs_tot , ec_tot |
|---|
| 231 | c h_vcol_tot-- total enthalpy of vertical air column |
|---|
| 232 | C (air with watter vapour, liquid and solid) (J/m2) |
|---|
| 233 | c h_dair_tot-- total enthalpy of dry air (J/m2) |
|---|
| 234 | c h_qw_tot---- total enthalpy of watter vapour (J/m2) |
|---|
| 235 | c h_ql_tot---- total enthalpy of liquid watter (J/m2) |
|---|
| 236 | c h_qs_tot---- total enthalpy of solid watter (J/m2) |
|---|
| 237 | c qw_tot------ total mass of watter vapour (kg/m2) |
|---|
| 238 | c ql_tot------ total mass of liquid watter (kg/m2) |
|---|
| 239 | c qs_tot------ total mass of solid watter (kg/m2) |
|---|
| 240 | c ec_tot------ total cinetic energy (kg/m2) |
|---|
| 241 | C |
|---|
| 242 | REAL zairm(klon,klev) ! layer air mass (kg/m2) |
|---|
| 243 | REAL zqw_col(klon) |
|---|
| 244 | REAL zql_col(klon) |
|---|
| 245 | REAL zqs_col(klon) |
|---|
| 246 | REAL zec_col(klon) |
|---|
| 247 | REAL zh_dair_col(klon) |
|---|
| 248 | REAL zh_qw_col(klon), zh_ql_col(klon), zh_qs_col(klon) |
|---|
| 249 | C |
|---|
| 250 | REAL d_h_dair, d_h_qw, d_h_ql, d_h_qs |
|---|
| 251 | C |
|---|
| 252 | REAL airetot, zcpvap, zcwat, zcice |
|---|
| 253 | C |
|---|
| 254 | INTEGER i, k |
|---|
| 255 | C |
|---|
| 256 | INTEGER ndiag ! max number of diagnostic in parallel |
|---|
| 257 | PARAMETER (ndiag=10) |
|---|
| 258 | integer pas(ndiag) |
|---|
| 259 | save pas |
|---|
| 260 | data pas/ndiag*0/ |
|---|
| [704] | 261 | c$OMP THREADPRIVATE(pas) |
|---|
| [524] | 262 | C |
|---|
| 263 | REAL h_vcol_pre(ndiag), h_dair_pre(ndiag), h_qw_pre(ndiag) |
|---|
| 264 | $ , h_ql_pre(ndiag), h_qs_pre(ndiag), qw_pre(ndiag) |
|---|
| 265 | $ , ql_pre(ndiag), qs_pre(ndiag) , ec_pre(ndiag) |
|---|
| 266 | SAVE h_vcol_pre, h_dair_pre, h_qw_pre, h_ql_pre |
|---|
| 267 | $ , h_qs_pre, qw_pre, ql_pre, qs_pre , ec_pre |
|---|
| [704] | 268 | c$OMP THREADPRIVATE(h_vcol_pre, h_dair_pre, h_qw_pre, h_ql_pre) |
|---|
| 269 | c$OMP THREADPRIVATE(h_qs_pre, qw_pre, ql_pre, qs_pre , ec_pre) |
|---|
| [524] | 270 | c====================================================================== |
|---|
| 271 | C |
|---|
| 272 | DO k = 1, klev |
|---|
| 273 | DO i = 1, klon |
|---|
| 274 | C layer air mass |
|---|
| 275 | zairm(i,k) = (paprs(i,k)-paprs(i,k+1))/RG |
|---|
| 276 | ENDDO |
|---|
| 277 | END DO |
|---|
| 278 | C |
|---|
| 279 | C Reset variables |
|---|
| 280 | DO i = 1, klon |
|---|
| 281 | zqw_col(i)=0. |
|---|
| 282 | zql_col(i)=0. |
|---|
| 283 | zqs_col(i)=0. |
|---|
| 284 | zec_col(i) = 0. |
|---|
| 285 | zh_dair_col(i) = 0. |
|---|
| 286 | zh_qw_col(i) = 0. |
|---|
| 287 | zh_ql_col(i) = 0. |
|---|
| 288 | zh_qs_col(i) = 0. |
|---|
| 289 | ENDDO |
|---|
| 290 | C |
|---|
| 291 | zcpvap=RCPV |
|---|
| 292 | zcwat=RCW |
|---|
| 293 | zcice=RCS |
|---|
| 294 | C |
|---|
| 295 | C Compute vertical sum for each atmospheric column |
|---|
| 296 | C ================================================ |
|---|
| 297 | DO k = 1, klev |
|---|
| 298 | DO i = 1, klon |
|---|
| 299 | C Watter mass |
|---|
| 300 | zqw_col(i) = zqw_col(i) + q(i,k)*zairm(i,k) |
|---|
| 301 | zql_col(i) = zql_col(i) + ql(i,k)*zairm(i,k) |
|---|
| 302 | zqs_col(i) = zqs_col(i) + qs(i,k)*zairm(i,k) |
|---|
| 303 | C Cinetic Energy |
|---|
| 304 | zec_col(i) = zec_col(i) |
|---|
| 305 | $ +0.5*(u(i,k)**2+v(i,k)**2)*zairm(i,k) |
|---|
| 306 | C Air enthalpy |
|---|
| 307 | zh_dair_col(i) = zh_dair_col(i) |
|---|
| 308 | $ + RCPD*(1.-q(i,k)-ql(i,k)-qs(i,k))*zairm(i,k)*t(i,k) |
|---|
| 309 | zh_qw_col(i) = zh_qw_col(i) |
|---|
| 310 | $ + zcpvap*q(i,k)*zairm(i,k)*t(i,k) |
|---|
| 311 | zh_ql_col(i) = zh_ql_col(i) |
|---|
| 312 | $ + zcwat*ql(i,k)*zairm(i,k)*t(i,k) |
|---|
| 313 | $ - RLVTT*ql(i,k)*zairm(i,k) |
|---|
| 314 | zh_qs_col(i) = zh_qs_col(i) |
|---|
| 315 | $ + zcice*qs(i,k)*zairm(i,k)*t(i,k) |
|---|
| 316 | $ - RLSTT*qs(i,k)*zairm(i,k) |
|---|
| 317 | |
|---|
| 318 | END DO |
|---|
| 319 | ENDDO |
|---|
| 320 | C |
|---|
| 321 | C Mean over the planete surface |
|---|
| 322 | C ============================= |
|---|
| 323 | qw_tot = 0. |
|---|
| 324 | ql_tot = 0. |
|---|
| 325 | qs_tot = 0. |
|---|
| 326 | ec_tot = 0. |
|---|
| 327 | h_vcol_tot = 0. |
|---|
| 328 | h_dair_tot = 0. |
|---|
| 329 | h_qw_tot = 0. |
|---|
| 330 | h_ql_tot = 0. |
|---|
| 331 | h_qs_tot = 0. |
|---|
| 332 | airetot=0. |
|---|
| 333 | C |
|---|
| 334 | do i=1,klon |
|---|
| 335 | qw_tot = qw_tot + zqw_col(i)*airephy(i) |
|---|
| 336 | ql_tot = ql_tot + zql_col(i)*airephy(i) |
|---|
| 337 | qs_tot = qs_tot + zqs_col(i)*airephy(i) |
|---|
| 338 | ec_tot = ec_tot + zec_col(i)*airephy(i) |
|---|
| 339 | h_dair_tot = h_dair_tot + zh_dair_col(i)*airephy(i) |
|---|
| 340 | h_qw_tot = h_qw_tot + zh_qw_col(i)*airephy(i) |
|---|
| 341 | h_ql_tot = h_ql_tot + zh_ql_col(i)*airephy(i) |
|---|
| 342 | h_qs_tot = h_qs_tot + zh_qs_col(i)*airephy(i) |
|---|
| 343 | airetot=airetot+airephy(i) |
|---|
| 344 | END DO |
|---|
| 345 | C |
|---|
| 346 | qw_tot = qw_tot/airetot |
|---|
| 347 | ql_tot = ql_tot/airetot |
|---|
| 348 | qs_tot = qs_tot/airetot |
|---|
| 349 | ec_tot = ec_tot/airetot |
|---|
| 350 | h_dair_tot = h_dair_tot/airetot |
|---|
| 351 | h_qw_tot = h_qw_tot/airetot |
|---|
| 352 | h_ql_tot = h_ql_tot/airetot |
|---|
| 353 | h_qs_tot = h_qs_tot/airetot |
|---|
| 354 | C |
|---|
| 355 | h_vcol_tot = h_dair_tot+h_qw_tot+h_ql_tot+h_qs_tot |
|---|
| 356 | C |
|---|
| 357 | C Compute the change of the atmospheric state compare to the one |
|---|
| 358 | C stored in "idiag2", and convert it in flux. THis computation |
|---|
| 359 | C is performed IF idiag2 /= 0 and IF it is not the first CALL |
|---|
| 360 | c for "idiag" |
|---|
| 361 | C =================================== |
|---|
| 362 | C |
|---|
| 363 | IF ( (idiag2.gt.0) .and. (pas(idiag2) .ne. 0) ) THEN |
|---|
| 364 | d_h_vcol = (h_vcol_tot - h_vcol_pre(idiag2) )/dtime |
|---|
| 365 | d_h_dair = (h_dair_tot- h_dair_pre(idiag2))/dtime |
|---|
| 366 | d_h_qw = (h_qw_tot - h_qw_pre(idiag2) )/dtime |
|---|
| 367 | d_h_ql = (h_ql_tot - h_ql_pre(idiag2) )/dtime |
|---|
| 368 | d_h_qs = (h_qs_tot - h_qs_pre(idiag2) )/dtime |
|---|
| 369 | d_qw = (qw_tot - qw_pre(idiag2) )/dtime |
|---|
| 370 | d_ql = (ql_tot - ql_pre(idiag2) )/dtime |
|---|
| 371 | d_qs = (qs_tot - qs_pre(idiag2) )/dtime |
|---|
| 372 | d_ec = (ec_tot - ec_pre(idiag2) )/dtime |
|---|
| 373 | d_qt = d_qw + d_ql + d_qs |
|---|
| 374 | ELSE |
|---|
| 375 | d_h_vcol = 0. |
|---|
| 376 | d_h_dair = 0. |
|---|
| 377 | d_h_qw = 0. |
|---|
| 378 | d_h_ql = 0. |
|---|
| 379 | d_h_qs = 0. |
|---|
| 380 | d_qw = 0. |
|---|
| 381 | d_ql = 0. |
|---|
| 382 | d_qs = 0. |
|---|
| 383 | d_ec = 0. |
|---|
| 384 | d_qt = 0. |
|---|
| 385 | ENDIF |
|---|
| 386 | C |
|---|
| 387 | IF (iprt.ge.2) THEN |
|---|
| 388 | WRITE(6,9000) tit,pas(idiag),d_qt,d_qw,d_ql,d_qs |
|---|
| 389 | 9000 format('Phys. Watter Mass Budget (kg/m2/s)',A15 |
|---|
| 390 | $ ,1i6,10(1pE14.6)) |
|---|
| 391 | WRITE(6,9001) tit,pas(idiag), d_h_vcol |
|---|
| 392 | 9001 format('Phys. Enthalpy Budget (W/m2) ',A15,1i6,10(F8.2)) |
|---|
| 393 | WRITE(6,9002) tit,pas(idiag), d_ec |
|---|
| 394 | 9002 format('Phys. Cinetic Energy Budget (W/m2) ',A15,1i6,10(F8.2)) |
|---|
| 395 | END IF |
|---|
| 396 | C |
|---|
| 397 | C Store the new atmospheric state in "idiag" |
|---|
| 398 | C |
|---|
| 399 | pas(idiag)=pas(idiag)+1 |
|---|
| 400 | h_vcol_pre(idiag) = h_vcol_tot |
|---|
| 401 | h_dair_pre(idiag) = h_dair_tot |
|---|
| 402 | h_qw_pre(idiag) = h_qw_tot |
|---|
| 403 | h_ql_pre(idiag) = h_ql_tot |
|---|
| 404 | h_qs_pre(idiag) = h_qs_tot |
|---|
| 405 | qw_pre(idiag) = qw_tot |
|---|
| 406 | ql_pre(idiag) = ql_tot |
|---|
| 407 | qs_pre(idiag) = qs_tot |
|---|
| 408 | ec_pre (idiag) = ec_tot |
|---|
| 409 | C |
|---|
| 410 | RETURN |
|---|
| 411 | END |
|---|
