1 |
jmc |
1.75 |
C $Header: /u/gcmpack/MITgcm_contrib/nesting_sannino/code_nest_merged/solve_for_pressure.F,v 1.3 2010/11/28 01:56:55 jmc Exp $ |
2 |
heimbach |
1.21 |
C $Name: $ |
3 |
cnh |
1.1 |
|
4 |
edhill |
1.39 |
#include "PACKAGES_CONFIG.h" |
5 |
adcroft |
1.5 |
#include "CPP_OPTIONS.h" |
6 |
cnh |
1.1 |
|
7 |
cnh |
1.27 |
CBOP |
8 |
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C !ROUTINE: SOLVE_FOR_PRESSURE |
9 |
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C !INTERFACE: |
10 |
jmc |
1.71 |
SUBROUTINE SOLVE_FOR_PRESSURE( myTime, myIter, myThid ) |
11 |
cnh |
1.27 |
|
12 |
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C !DESCRIPTION: \bv |
13 |
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C *==========================================================* |
14 |
jmc |
1.58 |
C | SUBROUTINE SOLVE_FOR_PRESSURE |
15 |
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C | o Controls inversion of two and/or three-dimensional |
16 |
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C | elliptic problems for the pressure field. |
17 |
cnh |
1.27 |
C *==========================================================* |
18 |
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C \ev |
19 |
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20 |
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C !USES: |
21 |
adcroft |
1.8 |
IMPLICIT NONE |
22 |
cnh |
1.4 |
C == Global variables |
23 |
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#include "SIZE.h" |
24 |
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#include "EEPARAMS.h" |
25 |
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#include "PARAMS.h" |
26 |
adcroft |
1.12 |
#include "GRID.h" |
27 |
jmc |
1.17 |
#include "SURFACE.h" |
28 |
jmc |
1.28 |
#include "FFIELDS.h" |
29 |
jmc |
1.48 |
#include "DYNVARS.h" |
30 |
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#include "SOLVE_FOR_PRESSURE.h" |
31 |
adcroft |
1.9 |
#ifdef ALLOW_NONHYDROSTATIC |
32 |
adcroft |
1.25 |
#include "SOLVE_FOR_PRESSURE3D.h" |
33 |
jmc |
1.48 |
#include "NH_VARS.h" |
34 |
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#endif |
35 |
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#ifdef ALLOW_CD_CODE |
36 |
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#include "CD_CODE_VARS.h" |
37 |
adcroft |
1.12 |
#endif |
38 |
adcroft |
1.11 |
#ifdef ALLOW_OBCS |
39 |
adcroft |
1.9 |
#include "OBCS.h" |
40 |
adcroft |
1.11 |
#endif |
41 |
cnh |
1.4 |
|
42 |
jmc |
1.32 |
C === Functions ==== |
43 |
jmc |
1.46 |
LOGICAL DIFFERENT_MULTIPLE |
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EXTERNAL DIFFERENT_MULTIPLE |
45 |
jmc |
1.32 |
|
46 |
cnh |
1.27 |
C !INPUT/OUTPUT PARAMETERS: |
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cnh |
1.1 |
C == Routine arguments == |
48 |
jmc |
1.58 |
C myTime :: Current time in simulation |
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C myIter :: Current iteration number in simulation |
50 |
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C myThid :: Thread number for this instance of SOLVE_FOR_PRESSURE |
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jmc |
1.28 |
_RL myTime |
52 |
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INTEGER myIter |
53 |
jmc |
1.29 |
INTEGER myThid |
54 |
cnh |
1.4 |
|
55 |
cnh |
1.27 |
C !LOCAL VARIABLES: |
56 |
adcroft |
1.22 |
C == Local variables == |
57 |
cnh |
1.6 |
INTEGER i,j,k,bi,bj |
58 |
jmc |
1.73 |
INTEGER ks |
59 |
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INTEGER numIters |
60 |
adcroft |
1.22 |
_RL firstResidual,lastResidual |
61 |
jmc |
1.36 |
_RL tmpFac |
62 |
jmc |
1.65 |
_RL sumEmP, tileEmP(nSx,nSy) |
63 |
jmc |
1.47 |
LOGICAL putPmEinXvector |
64 |
jmc |
1.73 |
INTEGER ioUnit |
65 |
jmc |
1.61 |
CHARACTER*10 sufx |
66 |
adcroft |
1.25 |
CHARACTER*(MAX_LEN_MBUF) msgBuf |
67 |
jmc |
1.49 |
#ifdef ALLOW_NONHYDROSTATIC |
68 |
jmc |
1.71 |
LOGICAL zeroPsNH, zeroMeanPnh, oldFreeSurfTerm |
69 |
jmc |
1.63 |
#else |
70 |
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_RL cg3d_b(1) |
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jmc |
1.49 |
#endif |
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cnh |
1.27 |
CEOP |
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jmc |
1.17 |
|
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jmc |
1.49 |
#ifdef ALLOW_NONHYDROSTATIC |
75 |
jmc |
1.68 |
zeroPsNH = .FALSE. |
76 |
jmc |
1.71 |
c zeroPsNH = use3Dsolver .AND. exactConserv |
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c & .AND. select_rStar.EQ.0 |
78 |
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zeroMeanPnh = .FALSE. |
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c zeroMeanPnh = use3Dsolver .AND. select_rStar.NE.0 |
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jmc |
1.72 |
c oldFreeSurfTerm = use3Dsolver .AND. select_rStar.EQ.0 |
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c & .AND. .NOT.zeroPsNH |
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oldFreeSurfTerm = use3Dsolver .AND. .NOT.exactConserv |
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jmc |
1.63 |
#else |
84 |
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cg3d_b(1) = 0. |
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jmc |
1.49 |
#endif |
86 |
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jmc |
1.58 |
C deepAtmosphere & useRealFreshWaterFlux: only valid if deepFac2F(ksurf)=1 |
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C anelastic (always Z-coordinate): |
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C 1) assume that rhoFacF(1)=1 (and ksurf == 1); |
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C (this reduces the number of lines of code to modify) |
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C 2) (a) 2-D continuity eq. compute div. of mass transport (<- add rhoFac) |
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C (b) gradient of surf.Press in momentum eq. (<- add 1/rhoFac) |
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C => 2 factors cancel in elliptic eq. for Phi_s , |
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C but 1rst factor(a) remains in RHS cg2d_b. |
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96 |
jmc |
1.47 |
C-- Initialise the Vector solution with etaN + deltaT*Global_mean_PmE |
97 |
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C instead of simply etaN ; This can speed-up the solver convergence in |
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C the case where |Global_mean_PmE| is large. |
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putPmEinXvector = .FALSE. |
100 |
jmc |
1.64 |
c putPmEinXvector = useRealFreshWaterFlux.AND.fluidIsWater |
101 |
jmc |
1.47 |
|
102 |
jmc |
1.71 |
IF ( myIter.EQ.1+nIter0 .AND. debugLevel .GE. debLevA ) THEN |
103 |
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_BEGIN_MASTER( myThid ) |
104 |
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ioUnit = standardMessageUnit |
105 |
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WRITE(msgBuf,'(2A,L5)') 'SOLVE_FOR_PRESSURE:', |
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& ' putPmEinXvector =', putPmEinXvector |
107 |
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CALL PRINT_MESSAGE( msgBuf, ioUnit, SQUEEZE_RIGHT, myThid ) |
108 |
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#ifdef ALLOW_NONHYDROSTATIC |
109 |
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WRITE(msgBuf,'(A,2(A,L5))') 'SOLVE_FOR_PRESSURE:', |
110 |
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& ' zeroPsNH=', zeroPsNH, ' , zeroMeanPnh=', zeroMeanPnh |
111 |
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CALL PRINT_MESSAGE( msgBuf, ioUnit, SQUEEZE_RIGHT, myThid ) |
112 |
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WRITE(msgBuf,'(2A,L5)') 'SOLVE_FOR_PRESSURE:', |
113 |
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& ' oldFreeSurfTerm =', oldFreeSurfTerm |
114 |
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CALL PRINT_MESSAGE( msgBuf, ioUnit, SQUEEZE_RIGHT, myThid ) |
115 |
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#endif |
116 |
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_END_MASTER( myThid ) |
117 |
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ENDIF |
118 |
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jmc |
1.17 |
C-- Save previous solution & Initialise Vector solution and source term : |
120 |
jmc |
1.47 |
sumEmP = 0. |
121 |
jmc |
1.17 |
DO bj=myByLo(myThid),myByHi(myThid) |
122 |
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DO bi=myBxLo(myThid),myBxHi(myThid) |
123 |
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DO j=1-OLy,sNy+OLy |
124 |
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DO i=1-OLx,sNx+OLx |
125 |
edhill |
1.40 |
#ifdef ALLOW_CD_CODE |
126 |
jmc |
1.17 |
etaNm1(i,j,bi,bj) = etaN(i,j,bi,bj) |
127 |
jmc |
1.26 |
#endif |
128 |
jmc |
1.18 |
cg2d_x(i,j,bi,bj) = Bo_surf(i,j,bi,bj)*etaN(i,j,bi,bj) |
129 |
jmc |
1.17 |
cg2d_b(i,j,bi,bj) = 0. |
130 |
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ENDDO |
131 |
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ENDDO |
132 |
jmc |
1.64 |
IF (useRealFreshWaterFlux.AND.fluidIsWater) THEN |
133 |
jmc |
1.62 |
tmpFac = freeSurfFac*mass2rUnit |
134 |
jmc |
1.58 |
IF (exactConserv) |
135 |
jmc |
1.62 |
& tmpFac = freeSurfFac*mass2rUnit*implicDiv2DFlow |
136 |
jmc |
1.29 |
DO j=1,sNy |
137 |
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DO i=1,sNx |
138 |
jmc |
1.58 |
cg2d_b(i,j,bi,bj) = |
139 |
jmc |
1.29 |
& tmpFac*_rA(i,j,bi,bj)*EmPmR(i,j,bi,bj)/deltaTMom |
140 |
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ENDDO |
141 |
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ENDDO |
142 |
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ENDIF |
143 |
jmc |
1.47 |
IF ( putPmEinXvector ) THEN |
144 |
jmc |
1.65 |
tileEmP(bi,bj) = 0. |
145 |
jmc |
1.47 |
DO j=1,sNy |
146 |
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DO i=1,sNx |
147 |
jmc |
1.67 |
tileEmP(bi,bj) = tileEmP(bi,bj) |
148 |
jmc |
1.65 |
& + rA(i,j,bi,bj)*EmPmR(i,j,bi,bj) |
149 |
jmc |
1.74 |
& *maskInC(i,j,bi,bj) |
150 |
jmc |
1.47 |
ENDDO |
151 |
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ENDDO |
152 |
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ENDIF |
153 |
jmc |
1.17 |
ENDDO |
154 |
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ENDDO |
155 |
jmc |
1.47 |
IF ( putPmEinXvector ) THEN |
156 |
jmc |
1.65 |
CALL GLOBAL_SUM_TILE_RL( tileEmP, sumEmP, myThid ) |
157 |
jmc |
1.47 |
ENDIF |
158 |
adcroft |
1.12 |
|
159 |
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DO bj=myByLo(myThid),myByHi(myThid) |
160 |
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DO bi=myBxLo(myThid),myBxHi(myThid) |
161 |
jmc |
1.47 |
IF ( putPmEinXvector ) THEN |
162 |
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tmpFac = 0. |
163 |
jmc |
1.62 |
IF (globalArea.GT.0.) tmpFac = |
164 |
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& freeSurfFac*deltaTfreesurf*mass2rUnit*sumEmP/globalArea |
165 |
jmc |
1.47 |
DO j=1,sNy |
166 |
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DO i=1,sNx |
167 |
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cg2d_x(i,j,bi,bj) = cg2d_x(i,j,bi,bj) |
168 |
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& - tmpFac*Bo_surf(i,j,bi,bj) |
169 |
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ENDDO |
170 |
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ENDDO |
171 |
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ENDIF |
172 |
jmc |
1.58 |
C- RHS: similar to the divergence of the vertically integrated mass transport: |
173 |
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C del_i { Sum_k [ rhoFac.(dr.hFac).(dy.deepFac).(u*) ] } / deltaT |
174 |
jmc |
1.63 |
DO k=Nr,1,-1 |
175 |
adcroft |
1.12 |
CALL CALC_DIV_GHAT( |
176 |
jmc |
1.63 |
I bi,bj,k, |
177 |
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U cg2d_b, cg3d_b, |
178 |
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I myThid ) |
179 |
adcroft |
1.12 |
ENDDO |
180 |
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ENDDO |
181 |
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ENDDO |
182 |
cnh |
1.4 |
|
183 |
adcroft |
1.12 |
DO bj=myByLo(myThid),myByHi(myThid) |
184 |
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DO bi=myBxLo(myThid),myBxHi(myThid) |
185 |
adcroft |
1.13 |
#ifdef ALLOW_NONHYDROSTATIC |
186 |
jmc |
1.71 |
IF ( oldFreeSurfTerm ) THEN |
187 |
jmc |
1.73 |
C-- Add source term arising from w=d/dt (p_s + p_nh) |
188 |
jmc |
1.28 |
DO j=1,sNy |
189 |
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DO i=1,sNx |
190 |
jmc |
1.51 |
ks = ksurfC(i,j,bi,bj) |
191 |
|
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IF ( ks.LE.Nr ) THEN |
192 |
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cg2d_b(i,j,bi,bj) = cg2d_b(i,j,bi,bj) |
193 |
jmc |
1.58 |
& -freeSurfFac*_rA(i,j,bi,bj)*deepFac2F(ks) |
194 |
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& /deltaTMom/deltaTfreesurf |
195 |
jmc |
1.28 |
& *( etaN(i,j,bi,bj) |
196 |
jmc |
1.59 |
& +phi_nh(i,j,ks,bi,bj)*recip_Bo(i,j,bi,bj) ) |
197 |
jmc |
1.51 |
cg3d_b(i,j,ks,bi,bj) = cg3d_b(i,j,ks,bi,bj) |
198 |
jmc |
1.58 |
& -freeSurfFac*_rA(i,j,bi,bj)*deepFac2F(ks) |
199 |
|
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& /deltaTMom/deltaTfreesurf |
200 |
jmc |
1.28 |
& *( etaN(i,j,bi,bj) |
201 |
jmc |
1.59 |
& +phi_nh(i,j,ks,bi,bj)*recip_Bo(i,j,bi,bj) ) |
202 |
jmc |
1.51 |
ENDIF |
203 |
jmc |
1.28 |
ENDDO |
204 |
adcroft |
1.12 |
ENDDO |
205 |
jmc |
1.28 |
ELSEIF ( exactConserv ) THEN |
206 |
adcroft |
1.13 |
#else |
207 |
jmc |
1.73 |
C-- Add source term arising from w=d/dt (p_s) |
208 |
jmc |
1.26 |
IF ( exactConserv ) THEN |
209 |
edhill |
1.39 |
#endif /* ALLOW_NONHYDROSTATIC */ |
210 |
jmc |
1.26 |
DO j=1,sNy |
211 |
|
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DO i=1,sNx |
212 |
jmc |
1.58 |
ks = ksurfC(i,j,bi,bj) |
213 |
jmc |
1.26 |
cg2d_b(i,j,bi,bj) = cg2d_b(i,j,bi,bj) |
214 |
jmc |
1.58 |
& -freeSurfFac*_rA(i,j,bi,bj)*deepFac2F(ks) |
215 |
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& /deltaTMom/deltaTfreesurf |
216 |
jmc |
1.26 |
& * etaH(i,j,bi,bj) |
217 |
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ENDDO |
218 |
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ENDDO |
219 |
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ELSE |
220 |
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DO j=1,sNy |
221 |
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DO i=1,sNx |
222 |
jmc |
1.58 |
ks = ksurfC(i,j,bi,bj) |
223 |
jmc |
1.26 |
cg2d_b(i,j,bi,bj) = cg2d_b(i,j,bi,bj) |
224 |
jmc |
1.58 |
& -freeSurfFac*_rA(i,j,bi,bj)*deepFac2F(ks) |
225 |
|
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& /deltaTMom/deltaTfreesurf |
226 |
jmc |
1.26 |
& * etaN(i,j,bi,bj) |
227 |
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ENDDO |
228 |
adcroft |
1.12 |
ENDDO |
229 |
jmc |
1.26 |
ENDIF |
230 |
adcroft |
1.12 |
|
231 |
|
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#ifdef ALLOW_OBCS |
232 |
adcroft |
1.14 |
IF (useOBCS) THEN |
233 |
adcroft |
1.12 |
DO i=1,sNx |
234 |
|
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C Northern boundary |
235 |
jmc |
1.63 |
IF (OB_Jn(i,bi,bj).NE.0) THEN |
236 |
|
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cg2d_b(i,OB_Jn(i,bi,bj),bi,bj)=0. |
237 |
|
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cg2d_x(i,OB_Jn(i,bi,bj),bi,bj)=0. |
238 |
adcroft |
1.12 |
ENDIF |
239 |
|
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C Southern boundary |
240 |
jmc |
1.63 |
IF (OB_Js(i,bi,bj).NE.0) THEN |
241 |
|
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cg2d_b(i,OB_Js(i,bi,bj),bi,bj)=0. |
242 |
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cg2d_x(i,OB_Js(i,bi,bj),bi,bj)=0. |
243 |
adcroft |
1.12 |
ENDIF |
244 |
|
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ENDDO |
245 |
jmc |
1.75 |
#ifndef ALLOW_NEST_CHILD |
246 |
adcroft |
1.12 |
DO j=1,sNy |
247 |
|
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C Eastern boundary |
248 |
jmc |
1.63 |
IF (OB_Ie(j,bi,bj).NE.0) THEN |
249 |
|
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cg2d_b(OB_Ie(j,bi,bj),j,bi,bj)=0. |
250 |
|
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cg2d_x(OB_Ie(j,bi,bj),j,bi,bj)=0. |
251 |
adcroft |
1.12 |
ENDIF |
252 |
|
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C Western boundary |
253 |
jmc |
1.63 |
IF (OB_Iw(j,bi,bj).NE.0) THEN |
254 |
|
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cg2d_b(OB_Iw(j,bi,bj),j,bi,bj)=0. |
255 |
|
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cg2d_x(OB_Iw(j,bi,bj),j,bi,bj)=0. |
256 |
adcroft |
1.12 |
ENDIF |
257 |
|
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ENDDO |
258 |
jmc |
1.75 |
#endif /* ALLOW_NEST_CHILD */ |
259 |
adcroft |
1.12 |
ENDIF |
260 |
jmc |
1.49 |
#endif /* ALLOW_OBCS */ |
261 |
|
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C- end bi,bj loops |
262 |
adcroft |
1.12 |
ENDDO |
263 |
|
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ENDDO |
264 |
|
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|
265 |
edhill |
1.42 |
#ifdef ALLOW_DEBUG |
266 |
heimbach |
1.38 |
IF ( debugLevel .GE. debLevB ) THEN |
267 |
adcroft |
1.23 |
CALL DEBUG_STATS_RL(1,cg2d_b,'cg2d_b (SOLVE_FOR_PRESSURE)', |
268 |
|
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& myThid) |
269 |
adcroft |
1.24 |
ENDIF |
270 |
adcroft |
1.23 |
#endif |
271 |
jmc |
1.61 |
IF ( DIFFERENT_MULTIPLE(diagFreq, myTime, deltaTClock) ) THEN |
272 |
|
|
WRITE(sufx,'(I10.10)') myIter |
273 |
jmc |
1.67 |
CALL WRITE_FLD_XY_RL( 'cg2d_b.', sufx, cg2d_b, myIter, myThid ) |
274 |
jmc |
1.61 |
ENDIF |
275 |
adcroft |
1.12 |
|
276 |
cnh |
1.1 |
C-- Find the surface pressure using a two-dimensional conjugate |
277 |
|
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C-- gradient solver. |
278 |
adcroft |
1.22 |
C see CG2D.h for the interface to this routine. |
279 |
|
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firstResidual=0. |
280 |
|
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lastResidual=0. |
281 |
adcroft |
1.19 |
numIters=cg2dMaxIters |
282 |
jmc |
1.50 |
c CALL TIMER_START('CG2D [SOLVE_FOR_PRESSURE]',myThid) |
283 |
heimbach |
1.56 |
#ifdef ALLOW_CG2D_NSA |
284 |
|
|
C-- Call the not-self-adjoint version of cg2d |
285 |
|
|
CALL CG2D_NSA( |
286 |
|
|
U cg2d_b, |
287 |
|
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U cg2d_x, |
288 |
|
|
O firstResidual, |
289 |
|
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O lastResidual, |
290 |
|
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U numIters, |
291 |
|
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I myThid ) |
292 |
|
|
#else /* not ALLOW_CG2D_NSA = default */ |
293 |
mlosch |
1.69 |
#ifdef ALLOW_SRCG |
294 |
|
|
IF ( useSRCGSolver ) THEN |
295 |
|
|
C-- Call the single reduce CG solver |
296 |
|
|
CALL CG2D_SR( |
297 |
adcroft |
1.22 |
U cg2d_b, |
298 |
cnh |
1.6 |
U cg2d_x, |
299 |
adcroft |
1.22 |
O firstResidual, |
300 |
|
|
O lastResidual, |
301 |
adcroft |
1.19 |
U numIters, |
302 |
cnh |
1.1 |
I myThid ) |
303 |
mlosch |
1.69 |
ELSE |
304 |
|
|
#else |
305 |
|
|
IF (.TRUE.) THEN |
306 |
|
|
C-- Call the default CG solver |
307 |
|
|
#endif /* ALLOW_SRCG */ |
308 |
|
|
CALL CG2D( |
309 |
|
|
U cg2d_b, |
310 |
|
|
U cg2d_x, |
311 |
|
|
O firstResidual, |
312 |
|
|
O lastResidual, |
313 |
|
|
U numIters, |
314 |
|
|
I myThid ) |
315 |
|
|
ENDIF |
316 |
heimbach |
1.56 |
#endif /* ALLOW_CG2D_NSA */ |
317 |
jmc |
1.67 |
_EXCH_XY_RL( cg2d_x, myThid ) |
318 |
jmc |
1.50 |
c CALL TIMER_STOP ('CG2D [SOLVE_FOR_PRESSURE]',myThid) |
319 |
adcroft |
1.23 |
|
320 |
edhill |
1.42 |
#ifdef ALLOW_DEBUG |
321 |
heimbach |
1.38 |
IF ( debugLevel .GE. debLevB ) THEN |
322 |
adcroft |
1.23 |
CALL DEBUG_STATS_RL(1,cg2d_x,'cg2d_x (SOLVE_FOR_PRESSURE)', |
323 |
|
|
& myThid) |
324 |
adcroft |
1.24 |
ENDIF |
325 |
adcroft |
1.23 |
#endif |
326 |
cnh |
1.1 |
|
327 |
jmc |
1.32 |
C- dump CG2D output at monitorFreq (to reduce size of STD-OUTPUT files) : |
328 |
jmc |
1.46 |
IF ( DIFFERENT_MULTIPLE(monitorFreq,myTime,deltaTClock) |
329 |
jmc |
1.45 |
& ) THEN |
330 |
heimbach |
1.38 |
IF ( debugLevel .GE. debLevA ) THEN |
331 |
|
|
_BEGIN_MASTER( myThid ) |
332 |
|
|
WRITE(msgBuf,'(A34,1PE24.14)') 'cg2d_init_res =',firstResidual |
333 |
|
|
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
334 |
|
|
WRITE(msgBuf,'(A34,I6)') 'cg2d_iters =',numIters |
335 |
|
|
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
336 |
|
|
WRITE(msgBuf,'(A34,1PE24.14)') 'cg2d_res =',lastResidual |
337 |
|
|
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
338 |
edhill |
1.43 |
_END_MASTER( myThid ) |
339 |
heimbach |
1.38 |
ENDIF |
340 |
jmc |
1.32 |
ENDIF |
341 |
jmc |
1.17 |
|
342 |
|
|
C-- Transfert the 2D-solution to "etaN" : |
343 |
|
|
DO bj=myByLo(myThid),myByHi(myThid) |
344 |
|
|
DO bi=myBxLo(myThid),myBxHi(myThid) |
345 |
|
|
DO j=1-OLy,sNy+OLy |
346 |
|
|
DO i=1-OLx,sNx+OLx |
347 |
jmc |
1.18 |
etaN(i,j,bi,bj) = recip_Bo(i,j,bi,bj)*cg2d_x(i,j,bi,bj) |
348 |
jmc |
1.17 |
ENDDO |
349 |
|
|
ENDDO |
350 |
|
|
ENDDO |
351 |
|
|
ENDDO |
352 |
adcroft |
1.10 |
|
353 |
adcroft |
1.9 |
#ifdef ALLOW_NONHYDROSTATIC |
354 |
jmc |
1.53 |
IF ( use3Dsolver ) THEN |
355 |
jmc |
1.67 |
IF ( DIFFERENT_MULTIPLE(diagFreq, myTime, deltaTClock) ) THEN |
356 |
|
|
WRITE(sufx,'(I10.10)') myIter |
357 |
|
|
CALL WRITE_FLD_XY_RL( 'cg2d_x.',sufx, cg2d_x, myIter, myThid ) |
358 |
|
|
ENDIF |
359 |
adcroft |
1.9 |
|
360 |
|
|
C-- Solve for a three-dimensional pressure term (NH or IGW or both ). |
361 |
|
|
C see CG3D.h for the interface to this routine. |
362 |
jmc |
1.71 |
|
363 |
jmc |
1.73 |
C-- Finish updating cg3d_b: 1) Add EmPmR contribution to top level cg3d_b: |
364 |
|
|
C 2) Update or Add free-surface contribution |
365 |
|
|
C 3) increment in horiz velocity due to new cg2d_x |
366 |
|
|
C 4) add vertical velocity contribution. |
367 |
|
|
CALL PRE_CG3D( |
368 |
|
|
I oldFreeSurfTerm, |
369 |
|
|
I cg2d_x, |
370 |
|
|
U cg3d_b, |
371 |
|
|
I myTime, myIter, myThid ) |
372 |
adcroft |
1.9 |
|
373 |
jmc |
1.67 |
#ifdef ALLOW_DEBUG |
374 |
jmc |
1.73 |
IF ( debugLevel .GE. debLevB ) THEN |
375 |
|
|
CALL DEBUG_STATS_RL(Nr,cg3d_b,'cg3d_b (SOLVE_FOR_PRESSURE)', |
376 |
|
|
& myThid) |
377 |
|
|
ENDIF |
378 |
jmc |
1.67 |
#endif |
379 |
|
|
IF ( DIFFERENT_MULTIPLE( diagFreq, myTime, deltaTClock) ) THEN |
380 |
|
|
WRITE(sufx,'(I10.10)') myIter |
381 |
jmc |
1.73 |
CALL WRITE_FLD_XYZ_RL('cg3d_b.',sufx, cg3d_b, myIter,myThid ) |
382 |
jmc |
1.67 |
ENDIF |
383 |
jmc |
1.49 |
|
384 |
jmc |
1.73 |
firstResidual=0. |
385 |
|
|
lastResidual=0. |
386 |
|
|
numIters=cg3dMaxIters |
387 |
|
|
CALL TIMER_START('CG3D [SOLVE_FOR_PRESSURE]',myThid) |
388 |
|
|
CALL CG3D( |
389 |
|
|
U cg3d_b, |
390 |
|
|
U phi_nh, |
391 |
|
|
O firstResidual, |
392 |
|
|
O lastResidual, |
393 |
|
|
U numIters, |
394 |
|
|
I myIter, myThid ) |
395 |
|
|
_EXCH_XYZ_RL( phi_nh, myThid ) |
396 |
|
|
CALL TIMER_STOP ('CG3D [SOLVE_FOR_PRESSURE]',myThid) |
397 |
|
|
|
398 |
|
|
IF ( DIFFERENT_MULTIPLE(monitorFreq,myTime,deltaTClock) |
399 |
|
|
& ) THEN |
400 |
|
|
IF ( debugLevel .GE. debLevA ) THEN |
401 |
|
|
_BEGIN_MASTER( myThid ) |
402 |
|
|
WRITE(msgBuf,'(A34,1PE24.14)') 'cg3d_init_res =',firstResidual |
403 |
|
|
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
404 |
|
|
WRITE(msgBuf,'(A34,I6)') 'cg3d_iters =',numIters |
405 |
|
|
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
406 |
|
|
WRITE(msgBuf,'(A34,1PE24.14)') 'cg3d_res =',lastResidual |
407 |
|
|
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
408 |
|
|
_END_MASTER( myThid ) |
409 |
|
|
ENDIF |
410 |
|
|
ENDIF |
411 |
jmc |
1.49 |
|
412 |
jmc |
1.73 |
C-- Separate the Hydrostatic Surface Pressure adjusment (=> put it in dPhiNH) |
413 |
|
|
C from the Non-hydrostatic pressure (since cg3d_x contains both contribution) |
414 |
|
|
IF ( nonHydrostatic .AND. exactConserv ) THEN |
415 |
|
|
IF ( DIFFERENT_MULTIPLE( diagFreq, myTime, deltaTClock) ) THEN |
416 |
|
|
WRITE(sufx,'(I10.10)') myIter |
417 |
|
|
CALL WRITE_FLD_XYZ_RL('cg3d_x.',sufx, phi_nh, myIter,myThid ) |
418 |
|
|
ENDIF |
419 |
|
|
CALL POST_CG3D( |
420 |
|
|
I zeroPsNH, zeroMeanPnh, |
421 |
|
|
I myTime, myIter, myThid ) |
422 |
|
|
ENDIF |
423 |
jmc |
1.49 |
|
424 |
|
|
ENDIF |
425 |
|
|
#endif /* ALLOW_NONHYDROSTATIC */ |
426 |
cnh |
1.1 |
|
427 |
heimbach |
1.60 |
#ifdef ALLOW_SHOWFLOPS |
428 |
|
|
CALL SHOWFLOPS_INSOLVE( myThid) |
429 |
ce107 |
1.52 |
#endif |
430 |
heimbach |
1.60 |
|
431 |
cnh |
1.1 |
RETURN |
432 |
|
|
END |