| 1 |
jmc |
1.1 |
C $Header: $ |
| 2 |
|
|
C $Name: $ |
| 3 |
|
|
|
| 4 |
|
|
#include "AIM_OPTIONS.h" |
| 5 |
|
|
|
| 6 |
|
|
CStartOfInterface |
| 7 |
|
|
SUBROUTINE AIM_AIM2DYN( |
| 8 |
|
|
I bi, bj, myTime, myIter, myThid) |
| 9 |
|
|
C *==========================================================* |
| 10 |
|
|
C | S/R AIM_AIM2DYN | |
| 11 |
|
|
C | o Remap AIM outputs to dynamics conforming arrays. | |
| 12 |
|
|
C |==========================================================* |
| 13 |
|
|
C | Currently AIM exports to the dynmaics | |
| 14 |
|
|
C | - PBL drag coefficient | |
| 15 |
|
|
C | - Net tendency for temperature | |
| 16 |
|
|
C | - Net tendency for water vapor | |
| 17 |
|
|
C | Exporting drag has the nice property that it is a scalar.| |
| 18 |
|
|
C | This means that the exchanges on the AIM exported fields | |
| 19 |
|
|
C | do not need special piaring on the cube. It may not be | |
| 20 |
|
|
C | a good idea in the long term as it makes assumptions | |
| 21 |
|
|
C | about the momentum schemes within AIM. | |
| 22 |
|
|
C *==========================================================* |
| 23 |
|
|
C------- |
| 24 |
|
|
C Note: Except LSC tendency, all others need to be /dpFac. |
| 25 |
|
|
C------- |
| 26 |
|
|
IMPLICIT NONE |
| 27 |
|
|
|
| 28 |
|
|
C == Global data == |
| 29 |
|
|
C-- size for MITgcm & Physics package : |
| 30 |
|
|
#include "AIM_SIZE.h" |
| 31 |
|
|
|
| 32 |
|
|
#include "EEPARAMS.h" |
| 33 |
|
|
#include "PARAMS.h" |
| 34 |
|
|
#include "GRID.h" |
| 35 |
|
|
#include "DYNVARS.h" |
| 36 |
|
|
|
| 37 |
|
|
#include "AIM2DYN.h" |
| 38 |
|
|
#include "com_physvar.h" |
| 39 |
|
|
|
| 40 |
|
|
C == Routine arguments == |
| 41 |
|
|
C bi,bj - Tile index |
| 42 |
|
|
C myTime - Current time of simulation ( s ) |
| 43 |
|
|
C myIter - Current iteration number in simulation |
| 44 |
|
|
C myThid - Number of this instance of the routine |
| 45 |
|
|
INTEGER bi, bj, myIter, myThid |
| 46 |
|
|
_RL myTime |
| 47 |
|
|
CEndOfInterface |
| 48 |
|
|
|
| 49 |
|
|
#ifdef ALLOW_AIM |
| 50 |
|
|
C == Local variables == |
| 51 |
|
|
C i,j,k :: loop counters |
| 52 |
|
|
C I2,Katm :: loop counters |
| 53 |
|
|
C conv_T2theta :: conversion factor from (absolute) Temp. to Pot.Temp. |
| 54 |
|
|
_RL conv_T2theta |
| 55 |
|
|
INTEGER i,j,k |
| 56 |
|
|
INTEGER I2, Katm |
| 57 |
|
|
|
| 58 |
|
|
C-- Physics tendency term |
| 59 |
|
|
|
| 60 |
|
|
DO k=1,Nr |
| 61 |
|
|
conv_T2theta = (atm_po/rC(k))**atm_kappa |
| 62 |
|
|
DO j=1,sNy |
| 63 |
|
|
DO i=1,sNx |
| 64 |
|
|
I2 = i+(j-1)*sNx |
| 65 |
|
|
Katm = _KD2KA( k ) |
| 66 |
|
|
C Planetary boundary layer drag coeff. |
| 67 |
|
|
aim_drag(i,j,bi,bj) = DRAG(I2,3,myThid) |
| 68 |
|
|
|
| 69 |
|
|
C Net temperature tendency |
| 70 |
|
|
aim_dTdt(i,j,k,bi,bj) = TT_LSC(I2,Katm,myThid) |
| 71 |
|
|
& + ( TT_CNV(I2,Katm,myThid) |
| 72 |
|
|
& +TT_PBL(I2,Katm,myThid) |
| 73 |
|
|
& +TT_RSW(I2,Katm,myThid) |
| 74 |
|
|
& +TT_RLW(I2,Katm,myThid) |
| 75 |
|
|
& )*recip_hFacC(i,j,k,bi,bj) |
| 76 |
|
|
aim_dTdt(i,j,k,bi,bj) = aim_dTdt(i,j,k,bi,bj)*conv_T2theta |
| 77 |
|
|
|
| 78 |
|
|
C Net water vapor tendency |
| 79 |
|
|
aim_dSdt(i,j,k,bi,bj) = QT_LSC(I2,Katm,myThid) |
| 80 |
|
|
& + ( QT_CNV(I2,Katm,myThid) |
| 81 |
|
|
& +QT_PBL(I2,Katm,myThid) |
| 82 |
|
|
& )*recip_hFacC(i,j,k,bi,bj) |
| 83 |
|
|
|
| 84 |
|
|
ENDDO |
| 85 |
|
|
ENDDO |
| 86 |
|
|
ENDDO |
| 87 |
|
|
|
| 88 |
|
|
#endif /* ALLOW_AIM */ |
| 89 |
|
|
|
| 90 |
|
|
RETURN |
| 91 |
|
|
END |
Parent Directory
| 
Revision Log
| 
Revision Graph