trunk/dyn3d/calfis.f

module calfis_m

  IMPLICIT NONE

contains

  SUBROUTINE calfis(rdayvrai, time, ucov, vcov, teta, q, pk, phis, phi, w, &
       dufi, dvfi, dtetafi, dqfi, lafin)

    ! From dyn3d/calfis.F, version 1.3, 2005/05/25 13:10:09
    ! Authors: P. Le Van, F. Hourdin

    ! 1. R\'earrangement des tableaux et transformation des variables
    ! dynamiques en variables physiques

    ! 2. Calcul des termes physiques
    ! 3. Retransformation des tendances physiques en tendances dynamiques

    ! Remarques:

    ! - Les vents sont donn\'es dans la physique par leurs composantes 
    ! naturelles.

    ! - La variable thermodynamique de la physique est une variable
    ! intensive : T.
    ! Pour la dynamique on prend T * (preff / p)**kappa

    ! - Les deux seules variables d\'ependant de la g\'eom\'etrie
    ! n\'ecessaires pour la physique sont la latitude (pour le
    ! rayonnement) et l'aire de la maille (quand on veut int\'egrer une
    ! grandeur horizontalement).

    use comconst, only: kappa, cpp, dtphys, g
    use comgeom, only: apoln, cu_2d, cv_2d, unsaire_2d, apols, rlonu, rlonv
    use dimens_m, only: iim, jjm, llm, nqmx
    use dimphy, only: klon
    use disvert_m, only: preff
    use grid_change, only: dyn_phy, gr_fi_dyn
    use nr_util, only: pi
    use physiq_m, only: physiq
    use pressure_var, only: p3d, pls

    REAL, intent(in):: rdayvrai
    REAL, intent(in):: time ! heure de la journ\'ee en fraction de jour

    REAL, intent(in):: ucov(:, :, :) ! (iim + 1, jjm + 1, llm) 
    ! covariant zonal velocity

    REAL, intent(in):: vcov(:, :, :) ! (iim + 1, jjm, llm) 
    !covariant meridional velocity 

    REAL, intent(in):: teta(:, :, :) ! (iim + 1, jjm + 1, llm)
    ! potential temperature

    REAL, intent(in):: q(:, :, :, :) ! (iim + 1, jjm + 1, llm, nqmx)
    ! mass fractions of advected fields

    REAL, intent(in):: pk(:, :, :) ! (iim + 1, jjm + 1, llm)
    ! Exner = cp * (p / preff)**kappa 

    REAL, intent(in):: phis(:, :) ! (iim + 1, jjm + 1)
    REAL, intent(in):: phi(:, :, :) ! (iim + 1, jjm + 1, llm)
    REAL, intent(in):: w(:, :, :) ! (iim + 1, jjm + 1, llm) in kg / s

    REAL, intent(out):: dufi(:, :, :) ! (iim + 1, jjm + 1, llm)
    ! tendency for the covariant zonal velocity (m2 s-2)

    REAL, intent(out):: dvfi(:, :, :) ! (iim + 1, jjm, llm)
    ! tendency for the natural meridional velocity

    REAL, intent(out):: dtetafi(:, :, :) ! (iim + 1, jjm + 1, llm)
    ! tendency for the potential temperature

    REAL, intent(out):: dqfi(:, :, :, :) ! (iim + 1, jjm + 1, llm, nqmx)
    LOGICAL, intent(in):: lafin

    ! Local:
    INTEGER i, j, l, ig0, iq
    REAL paprs(klon, llm + 1) ! aux interfaces des couches 
    REAL play(klon, llm) ! aux milieux des couches 
    REAL pphi(klon, llm), pphis(klon)
    REAL u(klon, llm), v(klon, llm)
    real zvfi(iim + 1, jjm + 1, llm)
    REAL t(klon, llm) ! temperature, in K
    real qx(klon, llm, nqmx) ! mass fractions of advected fields
    REAL omega(klon, llm)
    REAL d_u(klon, llm), d_v(klon, llm) ! tendances physiques du vent (m s-2)
    REAL d_t(klon, llm), d_qx(klon, llm, nqmx)
    REAL z1(iim)
    REAL pksurcp(iim + 1, jjm + 1)

    !-----------------------------------------------------------------------

    !!print *, "Call sequence information: calfis"

    ! 40. Transformation des variables dynamiques en variables physiques :

    ! 42. Pression intercouches :
    forall (l = 1: llm + 1) paprs(:, l) = pack(p3d(:, :, l), dyn_phy)

    ! 43. Température et pression milieu couche
    DO l = 1, llm
       pksurcp = pk(:, :, l) / cpp
       pls(:, :, l) = preff * pksurcp**(1./ kappa)
       play(:, l) = pack(pls(:, :, l), dyn_phy)
       t(:, l) = pack(teta(:, :, l) * pksurcp, dyn_phy)
    ENDDO

    ! 43.bis Traceurs :
    forall (iq = 1: nqmx, l = 1: llm) &
         qx(:, l, iq) = pack(q(:, :, l, iq), dyn_phy)

    ! Geopotentiel calcule par rapport a la surface locale :
    forall (l = 1 :llm) pphi(:, l) = pack(phi(:, :, l), dyn_phy)
    pphis = pack(phis, dyn_phy)
    forall (l = 1: llm) pphi(:, l) = pphi(:, l) - pphis

    ! Calcul de la vitesse verticale :
    forall (l = 1: llm)
       omega(1, l) = w(1, 1, l) * g / apoln
       omega(2: klon - 1, l) &
            = pack(w(:iim, 2: jjm, l) * g * unsaire_2d(:iim, 2: jjm), .true.)
       omega(klon, l) = w(1, jjm + 1, l) * g / apols
    END forall

    ! 45. champ u:

    DO l = 1, llm
       DO j = 2, jjm
          ig0 = 1 + (j - 2) * iim
          u(ig0 + 1, l) = 0.5 &
               * (ucov(iim, j, l) / cu_2d(iim, j) + ucov(1, j, l) / cu_2d(1, j))
          DO i = 2, iim
             u(ig0 + i, l) = 0.5 * (ucov(i - 1, j, l) / cu_2d(i - 1, j) &
                  + ucov(i, j, l) / cu_2d(i, j))
          end DO
       end DO
    end DO

    ! 46.champ v:

    forall (j = 2: jjm, l = 1: llm) zvfi(:iim, j, l) = 0.5 &
         * (vcov(:iim, j - 1, l) / cv_2d(:iim, j - 1) &
         + vcov(:iim, j, l) / cv_2d(:iim, j))
    zvfi(iim + 1, 2:jjm, :) = zvfi(1, 2:jjm, :)

    ! 47. champs de vents au p\^ole nord 
    ! U = 1 / pi * integrale [ v * cos(long) * d long ]
    ! V = 1 / pi * integrale [ v * sin(long) * d long ]

    DO l = 1, llm
       z1(1) = (rlonu(1) - rlonu(iim) + 2. * pi) * vcov(1, 1, l) / cv_2d(1, 1)
       DO i = 2, iim
          z1(i) = (rlonu(i) - rlonu(i - 1)) * vcov(i, 1, l) / cv_2d(i, 1)
       ENDDO

       u(1, l) = SUM(COS(rlonv(:iim)) * z1) / pi
       zvfi(:, 1, l) = SUM(SIN(rlonv(:iim)) * z1) / pi
    ENDDO

    ! 48. champs de vents au p\^ole sud:
    ! U = 1 / pi * integrale [ v * cos(long) * d long ]
    ! V = 1 / pi * integrale [ v * sin(long) * d long ]

    DO l = 1, llm
       z1(1) = (rlonu(1) - rlonu(iim) + 2. * pi) * vcov(1, jjm, l) &
            /cv_2d(1, jjm)
       DO i = 2, iim
          z1(i) = (rlonu(i) - rlonu(i - 1)) * vcov(i, jjm, l) / cv_2d(i, jjm)
       ENDDO

       u(klon, l) = SUM(COS(rlonv(:iim)) * z1) / pi
       zvfi(:, jjm + 1, l) = SUM(SIN(rlonv(:iim)) * z1) / pi
    ENDDO

    forall(l = 1: llm) v(:, l) = pack(zvfi(:, :, l), dyn_phy)

    ! Appel de la physique :
    CALL physiq(lafin, rdayvrai, time, dtphys, paprs, play, pphi, pphis, u, &
         v, t, qx, omega, d_u, d_v, d_t, d_qx)

    ! transformation des tendances physiques en tendances dynamiques:

    ! 62. enthalpie potentielle
    do l = 1, llm
       dtetafi(:, :, l) = cpp * gr_fi_dyn(d_t(:, l)) / pk(:, :, l)
    end do

    ! 63. traceurs
    DO iq = 1, nqmx
       DO l = 1, llm
          DO i = 1, iim + 1
             dqfi(i, 1, l, iq) = d_qx(1, l, iq)
             dqfi(i, jjm + 1, l, iq) = d_qx(klon, l, iq)
          ENDDO
          DO j = 2, jjm
             ig0 = 1 + (j - 2) * iim
             DO i = 1, iim
                dqfi(i, j, l, iq) = d_qx(ig0 + i, l, iq)
             ENDDO
             dqfi(iim + 1, j, l, iq) = dqfi(1, j, l, iq)
          ENDDO
       ENDDO
    ENDDO

    ! 65. champ u:
    DO l = 1, llm
       DO i = 1, iim + 1
          dufi(i, 1, l) = 0.
          dufi(i, jjm + 1, l) = 0.
       ENDDO

       DO j = 2, jjm
          ig0 = 1 + (j - 2) * iim
          DO i = 1, iim - 1
             dufi(i, j, l) = 0.5 * (d_u(ig0 + i, l) + d_u(ig0 + i+1, l)) &
                  * cu_2d(i, j)
          ENDDO
          dufi(iim, j, l) = 0.5 * (d_u(ig0 + 1, l) + d_u(ig0 + iim, l)) &
               * cu_2d(iim, j)
          dufi(iim + 1, j, l) = dufi(1, j, l)
       ENDDO
    ENDDO

    ! 67. champ v:

    DO l = 1, llm
       DO j = 2, jjm - 1
          ig0 = 1 + (j - 2) * iim
          DO i = 1, iim
             dvfi(i, j, l) = 0.5 * (d_v(ig0 + i, l) + d_v(ig0 + i+iim, l)) &
                  * cv_2d(i, j)
          ENDDO
          dvfi(iim + 1, j, l) = dvfi(1, j, l)
       ENDDO
    ENDDO

    ! 68. champ v pr\`es des p\^oles:
    ! v = U * cos(long) + V * SIN(long)

    DO l = 1, llm
       DO i = 1, iim
          dvfi(i, 1, l) = d_u(1, l) * COS(rlonv(i)) + d_v(1, l) * SIN(rlonv(i))
          dvfi(i, jjm, l) = d_u(klon, l) * COS(rlonv(i)) &
               + d_v(klon, l) * SIN(rlonv(i))
          dvfi(i, 1, l) = 0.5 * (dvfi(i, 1, l) + d_v(i + 1, l)) * cv_2d(i, 1)
          dvfi(i, jjm, l) = 0.5 &
               * (dvfi(i, jjm, l) + d_v(klon - iim - 1 + i, l)) * cv_2d(i, jjm)
       ENDDO

       dvfi(iim + 1, 1, l) = dvfi(1, 1, l)
       dvfi(iim + 1, jjm, l) = dvfi(1, jjm, l)
    ENDDO

  END SUBROUTINE calfis

end module calfis_m
1	module calfis_m
2
3	IMPLICIT NONE
4
5	contains
6
7	SUBROUTINE calfis(rdayvrai, time, ucov, vcov, teta, q, pk, phis, phi, w, &
8	dufi, dvfi, dtetafi, dqfi, lafin)
9
10	! From dyn3d/calfis.F, version 1.3, 2005/05/25 13:10:09
11	! Authors: P. Le Van, F. Hourdin
12
13	! 1. R\'earrangement des tableaux et transformation des variables
14	! dynamiques en variables physiques
15
16	! 2. Calcul des termes physiques
17	! 3. Retransformation des tendances physiques en tendances dynamiques
18
19	! Remarques:
20
21	! - Les vents sont donn\'es dans la physique par leurs composantes
22	! naturelles.
23
24	! - La variable thermodynamique de la physique est une variable
25	! intensive : T.
26	! Pour la dynamique on prend T * (preff / p)**kappa
27
28	! - Les deux seules variables d\'ependant de la g\'eom\'etrie
29	! n\'ecessaires pour la physique sont la latitude (pour le
30	! rayonnement) et l'aire de la maille (quand on veut int\'egrer une
31	! grandeur horizontalement).
32
33	use comconst, only: kappa, cpp, dtphys, g
34	use comgeom, only: apoln, cu_2d, cv_2d, unsaire_2d, apols, rlonu, rlonv
35	use dimens_m, only: iim, jjm, llm, nqmx
36	use dimphy, only: klon
37	use disvert_m, only: preff
38	use grid_change, only: dyn_phy, gr_fi_dyn
39	use nr_util, only: pi
40	use physiq_m, only: physiq
41	use pressure_var, only: p3d, pls
42
43	REAL, intent(in):: rdayvrai
44	REAL, intent(in):: time ! heure de la journ\'ee en fraction de jour
45
46	REAL, intent(in):: ucov(:, :, :) ! (iim + 1, jjm + 1, llm)
47	! covariant zonal velocity
48
49	REAL, intent(in):: vcov(:, :, :) ! (iim + 1, jjm, llm)
50	!covariant meridional velocity
51
52	REAL, intent(in):: teta(:, :, :) ! (iim + 1, jjm + 1, llm)
53	! potential temperature
54
55	REAL, intent(in):: q(:, :, :, :) ! (iim + 1, jjm + 1, llm, nqmx)
56	! mass fractions of advected fields
57
58	REAL, intent(in):: pk(:, :, :) ! (iim + 1, jjm + 1, llm)
59	! Exner = cp * (p / preff)**kappa
60
61	REAL, intent(in):: phis(:, :) ! (iim + 1, jjm + 1)
62	REAL, intent(in):: phi(:, :, :) ! (iim + 1, jjm + 1, llm)
63	REAL, intent(in):: w(:, :, :) ! (iim + 1, jjm + 1, llm) in kg / s
64
65	REAL, intent(out):: dufi(:, :, :) ! (iim + 1, jjm + 1, llm)
66	! tendency for the covariant zonal velocity (m2 s-2)
67
68	REAL, intent(out):: dvfi(:, :, :) ! (iim + 1, jjm, llm)
69	! tendency for the natural meridional velocity
70
71	REAL, intent(out):: dtetafi(:, :, :) ! (iim + 1, jjm + 1, llm)
72	! tendency for the potential temperature
73
74	REAL, intent(out):: dqfi(:, :, :, :) ! (iim + 1, jjm + 1, llm, nqmx)
75	LOGICAL, intent(in):: lafin
76
77	! Local:
78	INTEGER i, j, l, ig0, iq
79	REAL paprs(klon, llm + 1) ! aux interfaces des couches
80	REAL play(klon, llm) ! aux milieux des couches
81	REAL pphi(klon, llm), pphis(klon)
82	REAL u(klon, llm), v(klon, llm)
83	real zvfi(iim + 1, jjm + 1, llm)
84	REAL t(klon, llm) ! temperature, in K
85	real qx(klon, llm, nqmx) ! mass fractions of advected fields
86	REAL omega(klon, llm)
87	REAL d_u(klon, llm), d_v(klon, llm) ! tendances physiques du vent (m s-2)
88	REAL d_t(klon, llm), d_qx(klon, llm, nqmx)
89	REAL z1(iim)
90	REAL pksurcp(iim + 1, jjm + 1)
91
92	!-----------------------------------------------------------------------
93
94	!!print *, "Call sequence information: calfis"
95
96	! 40. Transformation des variables dynamiques en variables physiques :
97
98	! 42. Pression intercouches :
99	forall (l = 1: llm + 1) paprs(:, l) = pack(p3d(:, :, l), dyn_phy)
100
101	! 43. Température et pression milieu couche
102	DO l = 1, llm
103	pksurcp = pk(:, :, l) / cpp
104	pls(:, :, l) = preff * pksurcp**(1./ kappa)
105	play(:, l) = pack(pls(:, :, l), dyn_phy)
106	t(:, l) = pack(teta(:, :, l) * pksurcp, dyn_phy)
107	ENDDO
108
109	! 43.bis Traceurs :
110	forall (iq = 1: nqmx, l = 1: llm) &
111	qx(:, l, iq) = pack(q(:, :, l, iq), dyn_phy)
112
113	! Geopotentiel calcule par rapport a la surface locale :
114	forall (l = 1 :llm) pphi(:, l) = pack(phi(:, :, l), dyn_phy)
115	pphis = pack(phis, dyn_phy)
116	forall (l = 1: llm) pphi(:, l) = pphi(:, l) - pphis
117
118	! Calcul de la vitesse verticale :
119	forall (l = 1: llm)
120	omega(1, l) = w(1, 1, l) * g / apoln
121	omega(2: klon - 1, l) &
122	= pack(w(:iim, 2: jjm, l) * g * unsaire_2d(:iim, 2: jjm), .true.)
123	omega(klon, l) = w(1, jjm + 1, l) * g / apols
124	END forall
125
126	! 45. champ u:
127
128	DO l = 1, llm
129	DO j = 2, jjm
130	ig0 = 1 + (j - 2) * iim
131	u(ig0 + 1, l) = 0.5 &
132	* (ucov(iim, j, l) / cu_2d(iim, j) + ucov(1, j, l) / cu_2d(1, j))
133	DO i = 2, iim
134	u(ig0 + i, l) = 0.5 * (ucov(i - 1, j, l) / cu_2d(i - 1, j) &
135	+ ucov(i, j, l) / cu_2d(i, j))
136	end DO
137	end DO
138	end DO
139
140	! 46.champ v:
141
142	forall (j = 2: jjm, l = 1: llm) zvfi(:iim, j, l) = 0.5 &
143	* (vcov(:iim, j - 1, l) / cv_2d(:iim, j - 1) &
144	+ vcov(:iim, j, l) / cv_2d(:iim, j))
145	zvfi(iim + 1, 2:jjm, :) = zvfi(1, 2:jjm, :)
146
147	! 47. champs de vents au p\^ole nord
148	! U = 1 / pi * integrale [ v * cos(long) * d long ]
149	! V = 1 / pi * integrale [ v * sin(long) * d long ]
150
151	DO l = 1, llm
152	z1(1) = (rlonu(1) - rlonu(iim) + 2. * pi) * vcov(1, 1, l) / cv_2d(1, 1)
153	DO i = 2, iim
154	z1(i) = (rlonu(i) - rlonu(i - 1)) * vcov(i, 1, l) / cv_2d(i, 1)
155	ENDDO
156
157	u(1, l) = SUM(COS(rlonv(:iim)) * z1) / pi
158	zvfi(:, 1, l) = SUM(SIN(rlonv(:iim)) * z1) / pi
159	ENDDO
160
161	! 48. champs de vents au p\^ole sud:
162	! U = 1 / pi * integrale [ v * cos(long) * d long ]
163	! V = 1 / pi * integrale [ v * sin(long) * d long ]
164
165	DO l = 1, llm
166	z1(1) = (rlonu(1) - rlonu(iim) + 2. * pi) * vcov(1, jjm, l) &
167	/cv_2d(1, jjm)
168	DO i = 2, iim
169	z1(i) = (rlonu(i) - rlonu(i - 1)) * vcov(i, jjm, l) / cv_2d(i, jjm)
170	ENDDO
171
172	u(klon, l) = SUM(COS(rlonv(:iim)) * z1) / pi
173	zvfi(:, jjm + 1, l) = SUM(SIN(rlonv(:iim)) * z1) / pi
174	ENDDO
175
176	forall(l = 1: llm) v(:, l) = pack(zvfi(:, :, l), dyn_phy)
177
178	! Appel de la physique :
179	CALL physiq(lafin, rdayvrai, time, dtphys, paprs, play, pphi, pphis, u, &
180	v, t, qx, omega, d_u, d_v, d_t, d_qx)
181
182	! transformation des tendances physiques en tendances dynamiques:
183
184	! 62. enthalpie potentielle
185	do l = 1, llm
186	dtetafi(:, :, l) = cpp * gr_fi_dyn(d_t(:, l)) / pk(:, :, l)
187	end do
188
189	! 63. traceurs
190	DO iq = 1, nqmx
191	DO l = 1, llm
192	DO i = 1, iim + 1
193	dqfi(i, 1, l, iq) = d_qx(1, l, iq)
194	dqfi(i, jjm + 1, l, iq) = d_qx(klon, l, iq)
195	ENDDO
196	DO j = 2, jjm
197	ig0 = 1 + (j - 2) * iim
198	DO i = 1, iim
199	dqfi(i, j, l, iq) = d_qx(ig0 + i, l, iq)
200	ENDDO
201	dqfi(iim + 1, j, l, iq) = dqfi(1, j, l, iq)
202	ENDDO
203	ENDDO
204	ENDDO
205
206	! 65. champ u:
207	DO l = 1, llm
208	DO i = 1, iim + 1
209	dufi(i, 1, l) = 0.
210	dufi(i, jjm + 1, l) = 0.
211	ENDDO
212
213	DO j = 2, jjm
214	ig0 = 1 + (j - 2) * iim
215	DO i = 1, iim - 1
216	dufi(i, j, l) = 0.5 * (d_u(ig0 + i, l) + d_u(ig0 + i+1, l)) &
217	* cu_2d(i, j)
218	ENDDO
219	dufi(iim, j, l) = 0.5 * (d_u(ig0 + 1, l) + d_u(ig0 + iim, l)) &
220	* cu_2d(iim, j)
221	dufi(iim + 1, j, l) = dufi(1, j, l)
222	ENDDO
223	ENDDO
224
225	! 67. champ v:
226
227	DO l = 1, llm
228	DO j = 2, jjm - 1
229	ig0 = 1 + (j - 2) * iim
230	DO i = 1, iim
231	dvfi(i, j, l) = 0.5 * (d_v(ig0 + i, l) + d_v(ig0 + i+iim, l)) &
232	* cv_2d(i, j)
233	ENDDO
234	dvfi(iim + 1, j, l) = dvfi(1, j, l)
235	ENDDO
236	ENDDO
237
238	! 68. champ v pr\`es des p\^oles:
239	! v = U * cos(long) + V * SIN(long)
240
241	DO l = 1, llm
242	DO i = 1, iim
243	dvfi(i, 1, l) = d_u(1, l) * COS(rlonv(i)) + d_v(1, l) * SIN(rlonv(i))
244	dvfi(i, jjm, l) = d_u(klon, l) * COS(rlonv(i)) &
245	+ d_v(klon, l) * SIN(rlonv(i))
246	dvfi(i, 1, l) = 0.5 * (dvfi(i, 1, l) + d_v(i + 1, l)) * cv_2d(i, 1)
247	dvfi(i, jjm, l) = 0.5 &
248	* (dvfi(i, jjm, l) + d_v(klon - iim - 1 + i, l)) * cv_2d(i, jjm)
249	ENDDO
250
251	dvfi(iim + 1, 1, l) = dvfi(1, 1, l)
252	dvfi(iim + 1, jjm, l) = dvfi(1, jjm, l)
253	ENDDO
254
255	END SUBROUTINE calfis
256
257	end module calfis_m