Line |
Branch |
Exec |
Source |
1 |
|
✗ |
subroutine thermcell_dtke(ngrid,nlay,nsrf,ptimestep,fm0,entr0, & |
2 |
|
✗ |
& rg,pplev,tke) |
3 |
|
|
USE print_control_mod, ONLY: prt_level |
4 |
|
|
implicit none |
5 |
|
|
|
6 |
|
|
!======================================================================= |
7 |
|
|
! |
8 |
|
|
! Calcul du transport verticale dans la couche limite en presence |
9 |
|
|
! de "thermiques" explicitement representes |
10 |
|
|
! calcul du dq/dt une fois qu'on connait les ascendances |
11 |
|
|
! |
12 |
|
|
!======================================================================= |
13 |
|
|
|
14 |
|
|
integer ngrid,nlay,nsrf |
15 |
|
|
|
16 |
|
|
real ptimestep |
17 |
|
✗ |
real masse0(ngrid,nlay),fm0(ngrid,nlay+1),pplev(ngrid,nlay+1) |
18 |
|
|
real entr0(ngrid,nlay),rg |
19 |
|
|
real tke(ngrid,nlay,nsrf) |
20 |
|
✗ |
real detr0(ngrid,nlay) |
21 |
|
|
|
22 |
|
|
|
23 |
|
✗ |
real masse(ngrid,nlay),fm(ngrid,nlay+1) |
24 |
|
✗ |
real entr(ngrid,nlay) |
25 |
|
✗ |
real q(ngrid,nlay) |
26 |
|
|
integer lev_out ! niveau pour les print |
27 |
|
|
|
28 |
|
✗ |
real qa(ngrid,nlay),detr(ngrid,nlay),wqd(ngrid,nlay+1) |
29 |
|
|
|
30 |
|
|
real zzm |
31 |
|
|
|
32 |
|
|
integer ig,k |
33 |
|
|
integer isrf |
34 |
|
|
|
35 |
|
|
|
36 |
|
|
lev_out=0 |
37 |
|
|
|
38 |
|
|
|
39 |
|
✗ |
if (prt_level.ge.1) print*,'Q2 THERMCEL_DQ 0' |
40 |
|
|
|
41 |
|
|
! calcul du detrainement |
42 |
|
✗ |
do k=1,nlay |
43 |
|
✗ |
detr0(:,k)=fm0(:,k)-fm0(:,k+1)+entr0(:,k) |
44 |
|
✗ |
masse0(:,k)=(pplev(:,k)-pplev(:,k+1))/RG |
45 |
|
|
enddo |
46 |
|
|
|
47 |
|
|
|
48 |
|
|
! Decalage vertical des entrainements et detrainements. |
49 |
|
✗ |
masse(:,1)=0.5*masse0(:,1) |
50 |
|
✗ |
entr(:,1)=0.5*entr0(:,1) |
51 |
|
✗ |
detr(:,1)=0.5*detr0(:,1) |
52 |
|
✗ |
fm(:,1)=0. |
53 |
|
✗ |
do k=1,nlay-1 |
54 |
|
✗ |
masse(:,k+1)=0.5*(masse0(:,k)+masse0(:,k+1)) |
55 |
|
✗ |
entr(:,k+1)=0.5*(entr0(:,k)+entr0(:,k+1)) |
56 |
|
✗ |
detr(:,k+1)=0.5*(detr0(:,k)+detr0(:,k+1)) |
57 |
|
✗ |
fm(:,k+1)=fm(:,k)+entr(:,k)-detr(:,k) |
58 |
|
|
enddo |
59 |
|
✗ |
fm(:,nlay+1)=0. |
60 |
|
|
|
61 |
|
|
! calcul de la valeur dans les ascendances |
62 |
|
✗ |
do ig=1,ngrid |
63 |
|
✗ |
qa(ig,1)=q(ig,1) |
64 |
|
|
enddo |
65 |
|
|
|
66 |
|
|
|
67 |
|
|
|
68 |
|
✗ |
do isrf=1,nsrf |
69 |
|
|
|
70 |
|
✗ |
q(:,:)=tke(:,:,isrf) |
71 |
|
|
|
72 |
|
|
if (1==1) then |
73 |
|
✗ |
do k=2,nlay |
74 |
|
✗ |
do ig=1,ngrid |
75 |
|
✗ |
if ((fm(ig,k+1)+detr(ig,k))*ptimestep.gt. & |
76 |
|
|
& 1.e-5*masse(ig,k)) then |
77 |
|
|
qa(ig,k)=(fm(ig,k)*qa(ig,k-1)+entr(ig,k)*q(ig,k)) & |
78 |
|
✗ |
& /(fm(ig,k+1)+detr(ig,k)) |
79 |
|
|
else |
80 |
|
✗ |
qa(ig,k)=q(ig,k) |
81 |
|
|
endif |
82 |
|
|
if (qa(ig,k).lt.0.) then |
83 |
|
|
! print*,'qa<0!!!' |
84 |
|
|
endif |
85 |
|
✗ |
if (q(ig,k).lt.0.) then |
86 |
|
|
! print*,'q<0!!!' |
87 |
|
|
endif |
88 |
|
|
enddo |
89 |
|
|
enddo |
90 |
|
|
|
91 |
|
|
! Calcul du flux subsident |
92 |
|
|
|
93 |
|
✗ |
do k=2,nlay |
94 |
|
✗ |
do ig=1,ngrid |
95 |
|
✗ |
wqd(ig,k)=fm(ig,k)*q(ig,k) |
96 |
|
✗ |
if (wqd(ig,k).lt.0.) then |
97 |
|
|
! print*,'wqd<0!!!' |
98 |
|
|
endif |
99 |
|
|
enddo |
100 |
|
|
enddo |
101 |
|
✗ |
do ig=1,ngrid |
102 |
|
✗ |
wqd(ig,1)=0. |
103 |
|
✗ |
wqd(ig,nlay+1)=0. |
104 |
|
|
enddo |
105 |
|
|
|
106 |
|
|
|
107 |
|
|
! Calcul des tendances |
108 |
|
✗ |
do k=1,nlay |
109 |
|
✗ |
do ig=1,ngrid |
110 |
|
|
q(ig,k)=q(ig,k)+(detr(ig,k)*qa(ig,k)-entr(ig,k)*q(ig,k) & |
111 |
|
|
& -wqd(ig,k)+wqd(ig,k+1)) & |
112 |
|
✗ |
& *ptimestep/masse(ig,k) |
113 |
|
|
enddo |
114 |
|
|
enddo |
115 |
|
|
|
116 |
|
|
endif |
117 |
|
|
|
118 |
|
✗ |
tke(:,:,isrf)=q(:,:) |
119 |
|
|
|
120 |
|
|
enddo |
121 |
|
|
|
122 |
|
✗ |
return |
123 |
|
|
end |
124 |
|
|
|