| 1 |
module phystokenc_m |
| 2 |
|
| 3 |
IMPLICIT NONE |
| 4 |
|
| 5 |
contains |
| 6 |
|
| 7 |
SUBROUTINE phystokenc(pdtphys, rlon, rlat, pt, pmfu, pmfd, pen_u, pde_u, & |
| 8 |
pen_d, pde_d, pfm_therm, pentr_therm, pcoefh, yu1, yv1, ftsol, pctsrf, & |
| 9 |
frac_impa, frac_nucl, pphis, paire, dtime, itap) |
| 10 |
|
| 11 |
! From phylmd/phystokenc.F, version 1.2 2004/06/22 11:45:35 |
| 12 |
! Author: Fr\'ed\'eric Hourdin |
| 13 |
! Objet : \'ecriture des variables pour transport offline |
| 14 |
|
| 15 |
USE histwrite_m, ONLY: histwrite |
| 16 |
USE histsync_m, ONLY: histsync |
| 17 |
USE dimens_m, ONLY: iim, jjm, nqmx |
| 18 |
USE indicesol, ONLY: nbsrf |
| 19 |
use initphysto_m, only: initphysto |
| 20 |
USE dimphy, ONLY: klev, klon |
| 21 |
USE tracstoke, ONLY: istphy |
| 22 |
|
| 23 |
REAL, INTENT (IN):: pdtphys ! pas d'integration pour la physique (seconde) |
| 24 |
REAL, INTENT (IN):: rlon(klon), rlat(klon) |
| 25 |
REAL, intent(in):: pt(klon, klev) |
| 26 |
|
| 27 |
! convection: |
| 28 |
|
| 29 |
REAL, INTENT (IN):: pmfu(klon, klev) ! flux de masse dans le panache montant |
| 30 |
|
| 31 |
REAL, intent(in):: pmfd(klon, klev) |
| 32 |
! flux de masse dans le panache descendant |
| 33 |
|
| 34 |
REAL, intent(in):: pen_u(klon, klev) ! flux entraine dans le panache montant |
| 35 |
REAL, intent(in):: pde_u(klon, klev) ! flux detraine dans le panache montant |
| 36 |
|
| 37 |
REAL, intent(in):: pen_d(klon, klev) |
| 38 |
! flux entraine dans le panache descendant |
| 39 |
|
| 40 |
REAL, intent(in):: pde_d(klon, klev) |
| 41 |
! flux detraine dans le panache descendant |
| 42 |
|
| 43 |
! Les Thermiques |
| 44 |
REAL pfm_therm(klon, klev+1) |
| 45 |
REAL pentr_therm(klon, klev) |
| 46 |
|
| 47 |
! Couche limite: |
| 48 |
|
| 49 |
REAL pcoefh(klon, klev) ! coeff melange Couche limite |
| 50 |
REAL yu1(klon) |
| 51 |
REAL yv1(klon) |
| 52 |
|
| 53 |
! Arguments necessaires pour les sources et puits de traceur |
| 54 |
|
| 55 |
REAL ftsol(klon, nbsrf) ! Temperature du sol (surf)(Kelvin) |
| 56 |
REAL pctsrf(klon, nbsrf) ! Pourcentage de sol f(nature du sol) |
| 57 |
|
| 58 |
! Lessivage: |
| 59 |
|
| 60 |
REAL frac_impa(klon, klev) |
| 61 |
REAL frac_nucl(klon, klev) |
| 62 |
|
| 63 |
REAL, INTENT(IN):: pphis(klon) |
| 64 |
real paire(klon) |
| 65 |
REAL, INTENT (IN):: dtime |
| 66 |
INTEGER, INTENT (IN):: itap |
| 67 |
|
| 68 |
! Variables local to the procedure: |
| 69 |
|
| 70 |
real t(klon, klev) |
| 71 |
INTEGER, SAVE:: physid |
| 72 |
REAL zx_tmp_3d(iim, jjm+1, klev), zx_tmp_2d(iim, jjm+1) |
| 73 |
|
| 74 |
! Les Thermiques |
| 75 |
|
| 76 |
REAL fm_therm1(klon, klev) |
| 77 |
REAL entr_therm(klon, klev) |
| 78 |
REAL fm_therm(klon, klev) |
| 79 |
|
| 80 |
INTEGER i, k |
| 81 |
|
| 82 |
REAL, save:: mfu(klon, klev) ! flux de masse dans le panache montant |
| 83 |
REAL mfd(klon, klev) ! flux de masse dans le panache descendant |
| 84 |
REAL en_u(klon, klev) ! flux entraine dans le panache montant |
| 85 |
REAL de_u(klon, klev) ! flux detraine dans le panache montant |
| 86 |
REAL en_d(klon, klev) ! flux entraine dans le panache descendant |
| 87 |
REAL de_d(klon, klev) ! flux detraine dans le panache descendant |
| 88 |
REAL coefh(klon, klev) ! flux detraine dans le panache descendant |
| 89 |
|
| 90 |
REAL pyu1(klon), pyv1(klon) |
| 91 |
REAL pftsol(klon, nbsrf), ppsrf(klon, nbsrf) |
| 92 |
REAL pftsol1(klon), pftsol2(klon), pftsol3(klon), pftsol4(klon) |
| 93 |
REAL ppsrf1(klon), ppsrf2(klon), ppsrf3(klon), ppsrf4(klon) |
| 94 |
|
| 95 |
REAL dtcum |
| 96 |
|
| 97 |
INTEGER:: iadvtr = 0, irec = 1 |
| 98 |
REAL zmin, zmax |
| 99 |
LOGICAL ok_sync |
| 100 |
|
| 101 |
SAVE t, mfd, en_u, de_u, en_d, de_d, coefh, dtcum |
| 102 |
SAVE fm_therm, entr_therm |
| 103 |
SAVE pyu1, pyv1, pftsol, ppsrf |
| 104 |
|
| 105 |
!------------------------------------------------------ |
| 106 |
|
| 107 |
! Couche limite: |
| 108 |
|
| 109 |
ok_sync = .TRUE. |
| 110 |
|
| 111 |
IF (iadvtr==0) THEN |
| 112 |
CALL initphysto('phystoke', rlon, rlat, dtime, dtime*istphy, & |
| 113 |
dtime*istphy, physid) |
| 114 |
END IF |
| 115 |
|
| 116 |
i = itap |
| 117 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, pphis, zx_tmp_2d) |
| 118 |
CALL histwrite(physid, 'phis', i, zx_tmp_2d) |
| 119 |
|
| 120 |
i = itap |
| 121 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, paire, zx_tmp_2d) |
| 122 |
CALL histwrite(physid, 'aire', i, zx_tmp_2d) |
| 123 |
|
| 124 |
iadvtr = iadvtr + 1 |
| 125 |
|
| 126 |
IF (mod(iadvtr, istphy) == 1 .OR. istphy == 1) THEN |
| 127 |
PRINT *, 'reinitialisation des champs cumules a iadvtr =', iadvtr |
| 128 |
DO k = 1, klev |
| 129 |
DO i = 1, klon |
| 130 |
mfu(i, k) = 0. |
| 131 |
mfd(i, k) = 0. |
| 132 |
en_u(i, k) = 0. |
| 133 |
de_u(i, k) = 0. |
| 134 |
en_d(i, k) = 0. |
| 135 |
de_d(i, k) = 0. |
| 136 |
coefh(i, k) = 0. |
| 137 |
t(i, k) = 0. |
| 138 |
fm_therm(i, k) = 0. |
| 139 |
entr_therm(i, k) = 0. |
| 140 |
END DO |
| 141 |
END DO |
| 142 |
DO i = 1, klon |
| 143 |
pyv1(i) = 0. |
| 144 |
pyu1(i) = 0. |
| 145 |
END DO |
| 146 |
DO k = 1, nbsrf |
| 147 |
DO i = 1, klon |
| 148 |
pftsol(i, k) = 0. |
| 149 |
ppsrf(i, k) = 0. |
| 150 |
END DO |
| 151 |
END DO |
| 152 |
|
| 153 |
dtcum = 0. |
| 154 |
END IF |
| 155 |
|
| 156 |
DO k = 1, klev |
| 157 |
DO i = 1, klon |
| 158 |
mfu(i, k) = mfu(i, k) + pmfu(i, k)*pdtphys |
| 159 |
mfd(i, k) = mfd(i, k) + pmfd(i, k)*pdtphys |
| 160 |
en_u(i, k) = en_u(i, k) + pen_u(i, k)*pdtphys |
| 161 |
de_u(i, k) = de_u(i, k) + pde_u(i, k)*pdtphys |
| 162 |
en_d(i, k) = en_d(i, k) + pen_d(i, k)*pdtphys |
| 163 |
de_d(i, k) = de_d(i, k) + pde_d(i, k)*pdtphys |
| 164 |
coefh(i, k) = coefh(i, k) + pcoefh(i, k)*pdtphys |
| 165 |
t(i, k) = t(i, k) + pt(i, k)*pdtphys |
| 166 |
fm_therm(i, k) = fm_therm(i, k) + pfm_therm(i, k)*pdtphys |
| 167 |
entr_therm(i, k) = entr_therm(i, k) + pentr_therm(i, k)*pdtphys |
| 168 |
END DO |
| 169 |
END DO |
| 170 |
DO i = 1, klon |
| 171 |
pyv1(i) = pyv1(i) + yv1(i)*pdtphys |
| 172 |
pyu1(i) = pyu1(i) + yu1(i)*pdtphys |
| 173 |
END DO |
| 174 |
DO k = 1, nbsrf |
| 175 |
DO i = 1, klon |
| 176 |
pftsol(i, k) = pftsol(i, k) + ftsol(i, k)*pdtphys |
| 177 |
ppsrf(i, k) = ppsrf(i, k) + pctsrf(i, k)*pdtphys |
| 178 |
END DO |
| 179 |
END DO |
| 180 |
|
| 181 |
dtcum = dtcum + pdtphys |
| 182 |
|
| 183 |
IF (mod(iadvtr, istphy) == 0) THEN |
| 184 |
! normalisation par le temps cumule |
| 185 |
DO k = 1, klev |
| 186 |
DO i = 1, klon |
| 187 |
mfu(i, k) = mfu(i, k)/dtcum |
| 188 |
mfd(i, k) = mfd(i, k)/dtcum |
| 189 |
en_u(i, k) = en_u(i, k)/dtcum |
| 190 |
de_u(i, k) = de_u(i, k)/dtcum |
| 191 |
en_d(i, k) = en_d(i, k)/dtcum |
| 192 |
de_d(i, k) = de_d(i, k)/dtcum |
| 193 |
coefh(i, k) = coefh(i, k)/dtcum |
| 194 |
! Unitel a enlever |
| 195 |
t(i, k) = t(i, k)/dtcum |
| 196 |
fm_therm(i, k) = fm_therm(i, k)/dtcum |
| 197 |
entr_therm(i, k) = entr_therm(i, k)/dtcum |
| 198 |
END DO |
| 199 |
END DO |
| 200 |
DO i = 1, klon |
| 201 |
pyv1(i) = pyv1(i)/dtcum |
| 202 |
pyu1(i) = pyu1(i)/dtcum |
| 203 |
END DO |
| 204 |
DO k = 1, nbsrf |
| 205 |
DO i = 1, klon |
| 206 |
pftsol(i, k) = pftsol(i, k)/dtcum |
| 207 |
pftsol1(i) = pftsol(i, 1) |
| 208 |
pftsol2(i) = pftsol(i, 2) |
| 209 |
pftsol3(i) = pftsol(i, 3) |
| 210 |
pftsol4(i) = pftsol(i, 4) |
| 211 |
|
| 212 |
ppsrf(i, k) = ppsrf(i, k)/dtcum |
| 213 |
ppsrf1(i) = ppsrf(i, 1) |
| 214 |
ppsrf2(i) = ppsrf(i, 2) |
| 215 |
ppsrf3(i) = ppsrf(i, 3) |
| 216 |
ppsrf4(i) = ppsrf(i, 4) |
| 217 |
END DO |
| 218 |
END DO |
| 219 |
|
| 220 |
! ecriture des champs |
| 221 |
|
| 222 |
irec = irec + 1 |
| 223 |
|
| 224 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, t, zx_tmp_3d) |
| 225 |
CALL histwrite(physid, 't', itap, zx_tmp_3d) |
| 226 |
|
| 227 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, mfu, zx_tmp_3d) |
| 228 |
CALL histwrite(physid, 'mfu', itap, zx_tmp_3d) |
| 229 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, mfd, zx_tmp_3d) |
| 230 |
CALL histwrite(physid, 'mfd', itap, zx_tmp_3d) |
| 231 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, en_u, zx_tmp_3d) |
| 232 |
CALL histwrite(physid, 'en_u', itap, zx_tmp_3d) |
| 233 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, de_u, zx_tmp_3d) |
| 234 |
CALL histwrite(physid, 'de_u', itap, zx_tmp_3d) |
| 235 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, en_d, zx_tmp_3d) |
| 236 |
CALL histwrite(physid, 'en_d', itap, zx_tmp_3d) |
| 237 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, de_d, zx_tmp_3d) |
| 238 |
CALL histwrite(physid, 'de_d', itap, zx_tmp_3d) |
| 239 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, coefh, zx_tmp_3d) |
| 240 |
CALL histwrite(physid, 'coefh', itap, zx_tmp_3d) |
| 241 |
|
| 242 |
DO k = 1, klev |
| 243 |
DO i = 1, klon |
| 244 |
fm_therm1(i, k) = fm_therm(i, k) |
| 245 |
END DO |
| 246 |
END DO |
| 247 |
|
| 248 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, fm_therm1, zx_tmp_3d) |
| 249 |
CALL histwrite(physid, 'fm_th', itap, zx_tmp_3d) |
| 250 |
|
| 251 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, entr_therm, zx_tmp_3d) |
| 252 |
CALL histwrite(physid, 'en_th', itap, zx_tmp_3d) |
| 253 |
!ccc |
| 254 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, frac_impa, zx_tmp_3d) |
| 255 |
CALL histwrite(physid, 'frac_impa', itap, zx_tmp_3d) |
| 256 |
|
| 257 |
CALL gr_fi_ecrit(klev, klon, iim, jjm+1, frac_nucl, zx_tmp_3d) |
| 258 |
CALL histwrite(physid, 'frac_nucl', itap, zx_tmp_3d) |
| 259 |
|
| 260 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, pyu1, zx_tmp_2d) |
| 261 |
CALL histwrite(physid, 'pyu1', itap, zx_tmp_2d) |
| 262 |
|
| 263 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, pyv1, zx_tmp_2d) |
| 264 |
CALL histwrite(physid, 'pyv1', itap, zx_tmp_2d) |
| 265 |
|
| 266 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, pftsol1, zx_tmp_2d) |
| 267 |
CALL histwrite(physid, 'ftsol1', itap, zx_tmp_2d) |
| 268 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, pftsol2, zx_tmp_2d) |
| 269 |
CALL histwrite(physid, 'ftsol2', itap, zx_tmp_2d) |
| 270 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, pftsol3, zx_tmp_2d) |
| 271 |
CALL histwrite(physid, 'ftsol3', itap, zx_tmp_2d) |
| 272 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, pftsol4, zx_tmp_2d) |
| 273 |
CALL histwrite(physid, 'ftsol4', itap, zx_tmp_2d) |
| 274 |
|
| 275 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, ppsrf1, zx_tmp_2d) |
| 276 |
CALL histwrite(physid, 'psrf1', itap, zx_tmp_2d) |
| 277 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, ppsrf2, zx_tmp_2d) |
| 278 |
CALL histwrite(physid, 'psrf2', itap, zx_tmp_2d) |
| 279 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, ppsrf3, zx_tmp_2d) |
| 280 |
CALL histwrite(physid, 'psrf3', itap, zx_tmp_2d) |
| 281 |
CALL gr_fi_ecrit(1, klon, iim, jjm+1, ppsrf4, zx_tmp_2d) |
| 282 |
CALL histwrite(physid, 'psrf4', itap, zx_tmp_2d) |
| 283 |
|
| 284 |
IF (ok_sync) CALL histsync(physid) |
| 285 |
|
| 286 |
! Test sur la valeur des coefficients de lessivage |
| 287 |
|
| 288 |
zmin = 1E33 |
| 289 |
zmax = -1E33 |
| 290 |
DO k = 1, klev |
| 291 |
DO i = 1, klon |
| 292 |
zmax = max(zmax, frac_nucl(i, k)) |
| 293 |
zmin = min(zmin, frac_nucl(i, k)) |
| 294 |
END DO |
| 295 |
END DO |
| 296 |
PRINT *, 'coefs de lessivage (min et max)' |
| 297 |
PRINT *, 'facteur de nucleation ', zmin, zmax |
| 298 |
zmin = 1E33 |
| 299 |
zmax = -1E33 |
| 300 |
DO k = 1, klev |
| 301 |
DO i = 1, klon |
| 302 |
zmax = max(zmax, frac_impa(i, k)) |
| 303 |
zmin = min(zmin, frac_impa(i, k)) |
| 304 |
END DO |
| 305 |
END DO |
| 306 |
PRINT *, 'facteur d impaction ', zmin, zmax |
| 307 |
END IF |
| 308 |
|
| 309 |
END SUBROUTINE phystokenc |
| 310 |
|
| 311 |
end module phystokenc_m |
Parent Directory
| 
Revision Log