3 |
|
|
4 |
#include "CPP_OPTIONS.h" |
#include "CPP_OPTIONS.h" |
5 |
|
|
6 |
C /==========================================================\ |
CBOP |
7 |
C | S/R CALC_DIV_GHAT | |
C !ROUTINE: CALC_DIV_GHAT |
8 |
C | o Form the right hand-side of the surface pressure eqn. | |
C !INTERFACE: |
9 |
C |==========================================================| |
SUBROUTINE CALC_DIV_GHAT( |
10 |
C \==========================================================/ |
I bi,bj,k, |
11 |
SUBROUTINE CALC_DIV_GHAT( |
U cg2d_b, cg3d_b, |
12 |
I bi,bj,iMin,iMax,jMin,jMax,K, |
I myThid) |
13 |
I xA,yA, |
C !DESCRIPTION: \bv |
14 |
U cg2d_b, |
C *==========================================================* |
15 |
I myThid) |
C | S/R CALC_DIV_GHAT |
16 |
|
C | o Form the right hand-side of the surface pressure eqn. |
17 |
|
C *==========================================================* |
18 |
|
C | Right hand side of pressure equation is divergence |
19 |
|
C | of veclocity tendency (GHAT) term along with a relaxation |
20 |
|
C | term equal to the barotropic flow field divergence. |
21 |
|
C *==========================================================* |
22 |
|
C \ev |
23 |
|
|
24 |
|
C !USES: |
25 |
IMPLICIT NONE |
IMPLICIT NONE |
|
|
|
26 |
C == Global variables == |
C == Global variables == |
27 |
#include "SIZE.h" |
#include "SIZE.h" |
|
#include "DYNVARS.h" |
|
|
#include "FFIELDS.h" |
|
28 |
#include "EEPARAMS.h" |
#include "EEPARAMS.h" |
29 |
#include "PARAMS.h" |
#include "PARAMS.h" |
30 |
#include "GRID.h" |
#include "GRID.h" |
31 |
#include "SOLVE_FOR_PRESSURE3D.h" |
#include "DYNVARS.h" |
32 |
|
#ifdef ALLOW_ADDFLUID |
33 |
|
# include "FFIELDS.h" |
34 |
|
#endif |
35 |
|
|
36 |
|
C !INPUT/OUTPUT PARAMETERS: |
37 |
C == Routine arguments == |
C == Routine arguments == |
38 |
C bi, bj, iMin, iMax, jMin, jMax - Range of points for which calculation |
C bi, bj :: tile indices |
39 |
C results will be set. |
C k :: Index of layer. |
40 |
C k - Index of layer. |
C cg2d_b :: Conjugate Gradient 2-D solver : Right-hand side vector |
41 |
C xA, yA - Cell face areas |
C cg3d_b :: Conjugate Gradient 3-D solver : Right-hand side vector |
42 |
C cg2d_b - Conjugate Gradient 2-D solver : Right-hand side vector |
C myThid :: Instance number for this call of CALC_DIV_GHAT |
43 |
C myThid - Instance number for this call of CALC_DIV_GHAT |
INTEGER bi,bj |
44 |
INTEGER bi,bj,iMin,iMax,jMin,jMax |
INTEGER k |
|
INTEGER K |
|
|
_RS xA (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
|
|
_RS yA (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
|
45 |
_RL cg2d_b(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
_RL cg2d_b(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
46 |
|
#ifdef ALLOW_NONHYDROSTATIC |
47 |
|
_RL cg3d_b(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr,nSx,nSy) |
48 |
|
#else |
49 |
|
_RL cg3d_b(1) |
50 |
|
#endif |
51 |
INTEGER myThid |
INTEGER myThid |
52 |
|
|
53 |
|
C !LOCAL VARIABLES: |
54 |
C == Local variables == |
C == Local variables == |
55 |
|
C i,j :: Loop counters |
56 |
|
C xA, yA :: Cell vertical face areas |
57 |
|
C pf :: Intermediate array for building RHS source term. |
58 |
INTEGER i,j |
INTEGER i,j |
59 |
|
_RS xA (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
60 |
|
_RS yA (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
61 |
_RL pf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL pf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
62 |
|
CEOP |
63 |
|
|
64 |
|
C Calculate vertical face areas |
65 |
|
DO j=1,sNy+1 |
66 |
|
DO i=1,sNx+1 |
67 |
|
xA(i,j) = _dyG(i,j,bi,bj)*deepFacC(k) |
68 |
|
& *drF(k)*_hFacW(i,j,k,bi,bj)*rhoFacC(k) |
69 |
|
yA(i,j) = _dxG(i,j,bi,bj)*deepFacC(k) |
70 |
|
& *drF(k)*_hFacS(i,j,k,bi,bj)*rhoFacC(k) |
71 |
|
ENDDO |
72 |
|
ENDDO |
73 |
|
|
74 |
C-- Pressure equation source term |
C-- Pressure equation source term |
75 |
C Term is the vertical integral of the divergence of the |
C Term is the vertical integral of the divergence of the |
76 |
C time tendency terms along with a relaxation term that |
C time tendency terms along with a relaxation term that |
77 |
C pulls div(U) + dh/dt back toward zero. |
C pulls div(U) + dh/dt back toward zero. |
78 |
|
|
80 |
C Fully Implicit treatment of the Barotropic Flow Divergence |
C Fully Implicit treatment of the Barotropic Flow Divergence |
81 |
DO j=1,sNy |
DO j=1,sNy |
82 |
DO i=1,sNx+1 |
DO i=1,sNx+1 |
83 |
pf(i,j) = xA(i,j)*gUNm1(i,j,k,bi,bj) / deltaTmom |
pf(i,j) = xA(i,j)*gU(i,j,k,bi,bj) / deltaTMom |
84 |
ENDDO |
ENDDO |
85 |
ENDDO |
ENDDO |
86 |
ELSEIF (exactConserv) THEN |
ELSEIF (exactConserv) THEN |
88 |
C Implicit treatment of the Barotropic Flow Divergence |
C Implicit treatment of the Barotropic Flow Divergence |
89 |
DO j=1,sNy |
DO j=1,sNy |
90 |
DO i=1,sNx+1 |
DO i=1,sNx+1 |
91 |
pf(i,j) = implicDiv2Dflow |
pf(i,j) = implicDiv2Dflow |
92 |
& *xA(i,j)*gUNm1(i,j,k,bi,bj) / deltaTmom |
& *xA(i,j)*gU(i,j,k,bi,bj) / deltaTMom |
93 |
ENDDO |
ENDDO |
94 |
ENDDO |
ENDDO |
95 |
ELSE |
ELSE |
97 |
C => Filtering of uVel,vVel is necessary |
C => Filtering of uVel,vVel is necessary |
98 |
C-- Now the filter are applied in the_correction_step(). |
C-- Now the filter are applied in the_correction_step(). |
99 |
C We have left this code here to indicate where the filters used to be |
C We have left this code here to indicate where the filters used to be |
100 |
C in the algorithm before JMC moved them to after the pressure solver. |
C in the algorithm before JMC moved them to after the pressure solver. |
101 |
C- |
c#ifdef ALLOW_ZONAL_FILT |
102 |
C#ifdef ALLOW_ZONAL_FILT |
c IF (zonal_filt_lat.LT.90.) THEN |
103 |
C IF (zonal_filt_lat.LT.90.) THEN |
c CALL ZONAL_FILTER( |
104 |
C CALL ZONAL_FILTER( |
c U uVel( 1-OLx,1-OLy,k,bi,bj), |
105 |
C & uVel, hFacW, 1-1, sNy+1, k, k, bi, bj, 1, myThid) |
c I hFacW(1-OLx,1-OLy,k,bi,bj), |
106 |
C CALL ZONAL_FILTER( |
c I 0, sNy+1, 1, bi, bj, 1, myThid ) |
107 |
C & vVel, hFacS, 1-1, sNy+1, k, k, bi, bj, 2, myThid) |
c CALL ZONAL_FILTER( |
108 |
C ENDIF |
c U vVel( 1-OLx,1-OLy,k,bi,bj), |
109 |
C#endif |
c I hFacS(1-OLx,1-OLy,k,bi,bj), |
110 |
|
c I 0, sNy+1, 1, bi, bj, 2, myThid ) |
111 |
|
c ENDIF |
112 |
|
c#endif |
113 |
DO j=1,sNy |
DO j=1,sNy |
114 |
DO i=1,sNx+1 |
DO i=1,sNx+1 |
115 |
pf(i,j) = ( implicDiv2Dflow * gUNm1(i,j,k,bi,bj) |
pf(i,j) = ( implicDiv2Dflow * gU(i,j,k,bi,bj) |
116 |
& + (1.-implicDiv2Dflow) * uVel(i,j,k,bi,bj) |
& + (1. _d 0-implicDiv2Dflow)* uVel(i,j,k,bi,bj) |
117 |
& ) * xA(i,j) / deltaTmom |
& ) * xA(i,j) / deltaTMom |
118 |
ENDDO |
ENDDO |
119 |
ENDDO |
ENDDO |
120 |
ENDIF |
ENDIF |
126 |
ENDDO |
ENDDO |
127 |
|
|
128 |
#ifdef ALLOW_NONHYDROSTATIC |
#ifdef ALLOW_NONHYDROSTATIC |
129 |
IF (nonHydrostatic) THEN |
IF (use3Dsolver) THEN |
130 |
DO j=1,sNy |
DO j=1,sNy |
131 |
DO i=1,sNx |
DO i=1,sNx |
132 |
cg3d_b(i,j,k,bi,bj) = pf(i+1,j)-pf(i,j) |
cg3d_b(i,j,k,bi,bj) = ( pf(i+1,j)-pf(i,j) ) |
133 |
ENDDO |
ENDDO |
134 |
ENDDO |
ENDDO |
135 |
ENDIF |
ENDIF |
139 |
C Fully Implicit treatment of the Barotropic Flow Divergence |
C Fully Implicit treatment of the Barotropic Flow Divergence |
140 |
DO j=1,sNy+1 |
DO j=1,sNy+1 |
141 |
DO i=1,sNx |
DO i=1,sNx |
142 |
pf(i,j) = yA(i,j)*gVNm1(i,j,k,bi,bj) / deltatmom |
pf(i,j) = yA(i,j)*gV(i,j,k,bi,bj) / deltatmom |
143 |
ENDDO |
ENDDO |
144 |
ENDDO |
ENDDO |
145 |
ELSEIF (exactConserv) THEN |
ELSEIF (exactConserv) THEN |
148 |
DO j=1,sNy+1 |
DO j=1,sNy+1 |
149 |
DO i=1,sNx |
DO i=1,sNx |
150 |
pf(i,j) = implicDiv2Dflow |
pf(i,j) = implicDiv2Dflow |
151 |
& *yA(i,j)*gVNm1(i,j,k,bi,bj) / deltatmom |
& *yA(i,j)*gV(i,j,k,bi,bj) / deltatmom |
152 |
ENDDO |
ENDDO |
153 |
ENDDO |
ENDDO |
154 |
ELSE |
ELSE |
155 |
C Explicit+Implicit part of the Barotropic Flow Divergence |
C Explicit+Implicit part of the Barotropic Flow Divergence |
156 |
DO j=1,sNy+1 |
DO j=1,sNy+1 |
157 |
DO i=1,sNx |
DO i=1,sNx |
158 |
pf(i,j) = ( implicDiv2Dflow * gVNm1(i,j,k,bi,bj) |
pf(i,j) = ( implicDiv2Dflow * gV(i,j,k,bi,bj) |
159 |
& + (1.-implicDiv2Dflow) * vVel(i,j,k,bi,bj) |
& + (1. _d 0-implicDiv2Dflow)* vVel(i,j,k,bi,bj) |
160 |
& ) * yA(i,j) / deltaTmom |
& ) * yA(i,j) / deltaTMom |
161 |
ENDDO |
ENDDO |
162 |
ENDDO |
ENDDO |
163 |
ENDIF |
ENDIF |
169 |
ENDDO |
ENDDO |
170 |
|
|
171 |
#ifdef ALLOW_NONHYDROSTATIC |
#ifdef ALLOW_NONHYDROSTATIC |
172 |
IF (nonHydrostatic) THEN |
IF (use3Dsolver) THEN |
173 |
DO j=1,sNy |
DO j=1,sNy |
174 |
DO i=1,sNx |
DO i=1,sNx |
175 |
cg3d_b(i,j,k,bi,bj) = cg3d_b(i,j,k,bi,bj) + |
cg3d_b(i,j,k,bi,bj) = cg3d_b(i,j,k,bi,bj) |
176 |
& pf(i,j+1)-pf(i,j) |
& + ( pf(i,j+1)-pf(i,j) ) |
177 |
ENDDO |
ENDDO |
178 |
ENDDO |
ENDDO |
179 |
ENDIF |
ENDIF |
180 |
#endif |
#endif |
181 |
|
|
182 |
|
#ifdef ALLOW_ADDFLUID |
183 |
|
IF ( selectAddFluid.GE.1 ) THEN |
184 |
|
DO j=1,sNy |
185 |
|
DO i=1,sNx |
186 |
|
cg2d_b(i,j,bi,bj) = cg2d_b(i,j,bi,bj) |
187 |
|
& - addMass(i,j,k,bi,bj)*mass2rUnit/deltaTMom |
188 |
|
ENDDO |
189 |
|
ENDDO |
190 |
|
#ifdef ALLOW_NONHYDROSTATIC |
191 |
|
IF (use3Dsolver) THEN |
192 |
|
DO j=1,sNy |
193 |
|
DO i=1,sNx |
194 |
|
cg3d_b(i,j,k,bi,bj) = cg3d_b(i,j,k,bi,bj) |
195 |
|
& - addMass(i,j,k,bi,bj)*mass2rUnit/deltaTMom |
196 |
|
ENDDO |
197 |
|
ENDDO |
198 |
|
ENDIF |
199 |
|
#endif |
200 |
|
ENDIF |
201 |
|
#endif /* ALLOW_ADDFLUID */ |
202 |
|
|
203 |
RETURN |
RETURN |
204 |
END |
END |