1 |
jmc |
1.83 |
C $Header: /u/gcmpack/MITgcm/model/src/solve_for_pressure.F,v 1.82 2016/05/28 23:25:55 jmc Exp $ |
2 |
heimbach |
1.21 |
C $Name: $ |
3 |
cnh |
1.1 |
|
4 |
edhill |
1.39 |
#include "PACKAGES_CONFIG.h" |
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adcroft |
1.5 |
#include "CPP_OPTIONS.h" |
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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 |
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12 |
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C !DESCRIPTION: \bv |
13 |
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C *==========================================================* |
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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. |
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cnh |
1.27 |
C *==========================================================* |
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C \ev |
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C !USES: |
21 |
adcroft |
1.8 |
IMPLICIT NONE |
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cnh |
1.4 |
C == Global variables |
23 |
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#include "SIZE.h" |
24 |
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#include "EEPARAMS.h" |
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#include "PARAMS.h" |
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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" |
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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 |
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#ifdef ALLOW_CD_CODE |
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#include "CD_CODE_VARS.h" |
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adcroft |
1.12 |
#endif |
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cnh |
1.4 |
|
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jmc |
1.32 |
C === Functions ==== |
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jmc |
1.46 |
LOGICAL DIFFERENT_MULTIPLE |
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EXTERNAL DIFFERENT_MULTIPLE |
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jmc |
1.82 |
#ifdef ALLOW_DIAGNOSTICS |
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LOGICAL DIAGNOSTICS_IS_ON |
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EXTERNAL DIAGNOSTICS_IS_ON |
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#endif /* ALLOW_DIAGNOSTICS */ |
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jmc |
1.32 |
|
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cnh |
1.27 |
C !INPUT/OUTPUT PARAMETERS: |
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cnh |
1.1 |
C == Routine arguments == |
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jmc |
1.58 |
C myTime :: Current time in simulation |
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C myIter :: Current iteration number in simulation |
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C myThid :: Thread number for this instance of SOLVE_FOR_PRESSURE |
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jmc |
1.28 |
_RL myTime |
53 |
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INTEGER myIter |
54 |
jmc |
1.29 |
INTEGER myThid |
55 |
cnh |
1.4 |
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56 |
cnh |
1.27 |
C !LOCAL VARIABLES: |
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adcroft |
1.22 |
C == Local variables == |
58 |
cnh |
1.6 |
INTEGER i,j,k,bi,bj |
59 |
jmc |
1.73 |
INTEGER ks |
60 |
jmc |
1.79 |
INTEGER numIters, nIterMin |
61 |
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_RL firstResidual, minResidualSq, lastResidual |
62 |
jmc |
1.36 |
_RL tmpFac |
63 |
jmc |
1.65 |
_RL sumEmP, tileEmP(nSx,nSy) |
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jmc |
1.47 |
LOGICAL putPmEinXvector |
65 |
jmc |
1.73 |
INTEGER ioUnit |
66 |
adcroft |
1.25 |
CHARACTER*(MAX_LEN_MBUF) msgBuf |
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jmc |
1.49 |
#ifdef ALLOW_NONHYDROSTATIC |
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jmc |
1.71 |
LOGICAL zeroPsNH, zeroMeanPnh, oldFreeSurfTerm |
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jmc |
1.63 |
#else |
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_RL cg3d_b(1) |
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jmc |
1.49 |
#endif |
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jmc |
1.82 |
#ifdef ALLOW_DIAGNOSTICS |
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CHARACTER*8 diagName |
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_RL tmpVar (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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#endif /* ALLOW_DIAGNOSTICS */ |
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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 |
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jmc |
1.68 |
zeroPsNH = .FALSE. |
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jmc |
1.71 |
c zeroPsNH = use3Dsolver .AND. exactConserv |
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c & .AND. select_rStar.EQ.0 |
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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 |
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cg3d_b(1) = 0. |
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jmc |
1.49 |
#endif |
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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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jmc |
1.47 |
C-- Initialise the Vector solution with etaN + deltaT*Global_mean_PmE |
101 |
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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. |
104 |
jmc |
1.64 |
c putPmEinXvector = useRealFreshWaterFlux.AND.fluidIsWater |
105 |
jmc |
1.47 |
|
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jmc |
1.71 |
IF ( myIter.EQ.1+nIter0 .AND. debugLevel .GE. debLevA ) THEN |
107 |
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_BEGIN_MASTER( myThid ) |
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ioUnit = standardMessageUnit |
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WRITE(msgBuf,'(2A,L5)') 'SOLVE_FOR_PRESSURE:', |
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& ' putPmEinXvector =', putPmEinXvector |
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CALL PRINT_MESSAGE( msgBuf, ioUnit, SQUEEZE_RIGHT, myThid ) |
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#ifdef ALLOW_NONHYDROSTATIC |
113 |
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WRITE(msgBuf,'(A,2(A,L5))') 'SOLVE_FOR_PRESSURE:', |
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& ' zeroPsNH=', zeroPsNH, ' , zeroMeanPnh=', zeroMeanPnh |
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CALL PRINT_MESSAGE( msgBuf, ioUnit, SQUEEZE_RIGHT, myThid ) |
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WRITE(msgBuf,'(2A,L5)') 'SOLVE_FOR_PRESSURE:', |
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& ' oldFreeSurfTerm =', oldFreeSurfTerm |
118 |
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CALL PRINT_MESSAGE( msgBuf, ioUnit, SQUEEZE_RIGHT, myThid ) |
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#endif |
120 |
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_END_MASTER( myThid ) |
121 |
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ENDIF |
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jmc |
1.17 |
C-- Save previous solution & Initialise Vector solution and source term : |
124 |
jmc |
1.47 |
sumEmP = 0. |
125 |
jmc |
1.17 |
DO bj=myByLo(myThid),myByHi(myThid) |
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DO bi=myBxLo(myThid),myBxHi(myThid) |
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DO j=1-OLy,sNy+OLy |
128 |
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DO i=1-OLx,sNx+OLx |
129 |
edhill |
1.40 |
#ifdef ALLOW_CD_CODE |
130 |
jmc |
1.17 |
etaNm1(i,j,bi,bj) = etaN(i,j,bi,bj) |
131 |
jmc |
1.26 |
#endif |
132 |
jmc |
1.18 |
cg2d_x(i,j,bi,bj) = Bo_surf(i,j,bi,bj)*etaN(i,j,bi,bj) |
133 |
jmc |
1.17 |
cg2d_b(i,j,bi,bj) = 0. |
134 |
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ENDDO |
135 |
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ENDDO |
136 |
jmc |
1.64 |
IF (useRealFreshWaterFlux.AND.fluidIsWater) THEN |
137 |
jmc |
1.78 |
tmpFac = freeSurfFac*mass2rUnit*implicDiv2DFlow |
138 |
jmc |
1.29 |
DO j=1,sNy |
139 |
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DO i=1,sNx |
140 |
jmc |
1.58 |
cg2d_b(i,j,bi,bj) = |
141 |
jmc |
1.29 |
& tmpFac*_rA(i,j,bi,bj)*EmPmR(i,j,bi,bj)/deltaTMom |
142 |
jmc |
1.78 |
& *maskInC(i,j,bi,bj) |
143 |
jmc |
1.29 |
ENDDO |
144 |
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ENDDO |
145 |
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ENDIF |
146 |
jmc |
1.47 |
IF ( putPmEinXvector ) THEN |
147 |
jmc |
1.65 |
tileEmP(bi,bj) = 0. |
148 |
jmc |
1.47 |
DO j=1,sNy |
149 |
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DO i=1,sNx |
150 |
jmc |
1.67 |
tileEmP(bi,bj) = tileEmP(bi,bj) |
151 |
jmc |
1.65 |
& + rA(i,j,bi,bj)*EmPmR(i,j,bi,bj) |
152 |
jmc |
1.74 |
& *maskInC(i,j,bi,bj) |
153 |
jmc |
1.47 |
ENDDO |
154 |
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ENDDO |
155 |
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ENDIF |
156 |
jmc |
1.17 |
ENDDO |
157 |
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ENDDO |
158 |
jmc |
1.47 |
IF ( putPmEinXvector ) THEN |
159 |
jmc |
1.65 |
CALL GLOBAL_SUM_TILE_RL( tileEmP, sumEmP, myThid ) |
160 |
jmc |
1.47 |
ENDIF |
161 |
adcroft |
1.12 |
|
162 |
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DO bj=myByLo(myThid),myByHi(myThid) |
163 |
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DO bi=myBxLo(myThid),myBxHi(myThid) |
164 |
jmc |
1.47 |
IF ( putPmEinXvector ) THEN |
165 |
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tmpFac = 0. |
166 |
jmc |
1.62 |
IF (globalArea.GT.0.) tmpFac = |
167 |
jmc |
1.81 |
& freeSurfFac*deltaTFreeSurf*mass2rUnit*sumEmP/globalArea |
168 |
jmc |
1.47 |
DO j=1,sNy |
169 |
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DO i=1,sNx |
170 |
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cg2d_x(i,j,bi,bj) = cg2d_x(i,j,bi,bj) |
171 |
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& - tmpFac*Bo_surf(i,j,bi,bj) |
172 |
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ENDDO |
173 |
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ENDDO |
174 |
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ENDIF |
175 |
jmc |
1.58 |
C- RHS: similar to the divergence of the vertically integrated mass transport: |
176 |
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C del_i { Sum_k [ rhoFac.(dr.hFac).(dy.deepFac).(u*) ] } / deltaT |
177 |
jmc |
1.63 |
DO k=Nr,1,-1 |
178 |
adcroft |
1.12 |
CALL CALC_DIV_GHAT( |
179 |
jmc |
1.63 |
I bi,bj,k, |
180 |
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U cg2d_b, cg3d_b, |
181 |
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I myThid ) |
182 |
adcroft |
1.12 |
ENDDO |
183 |
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ENDDO |
184 |
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ENDDO |
185 |
cnh |
1.4 |
|
186 |
adcroft |
1.12 |
DO bj=myByLo(myThid),myByHi(myThid) |
187 |
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DO bi=myBxLo(myThid),myBxHi(myThid) |
188 |
adcroft |
1.13 |
#ifdef ALLOW_NONHYDROSTATIC |
189 |
jmc |
1.71 |
IF ( oldFreeSurfTerm ) THEN |
190 |
jmc |
1.73 |
C-- Add source term arising from w=d/dt (p_s + p_nh) |
191 |
jmc |
1.28 |
DO j=1,sNy |
192 |
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DO i=1,sNx |
193 |
jmc |
1.77 |
ks = kSurfC(i,j,bi,bj) |
194 |
jmc |
1.51 |
IF ( ks.LE.Nr ) THEN |
195 |
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cg2d_b(i,j,bi,bj) = cg2d_b(i,j,bi,bj) |
196 |
jmc |
1.58 |
& -freeSurfFac*_rA(i,j,bi,bj)*deepFac2F(ks) |
197 |
jmc |
1.81 |
& /deltaTMom/deltaTFreeSurf |
198 |
jmc |
1.28 |
& *( etaN(i,j,bi,bj) |
199 |
jmc |
1.59 |
& +phi_nh(i,j,ks,bi,bj)*recip_Bo(i,j,bi,bj) ) |
200 |
jmc |
1.51 |
cg3d_b(i,j,ks,bi,bj) = cg3d_b(i,j,ks,bi,bj) |
201 |
jmc |
1.58 |
& -freeSurfFac*_rA(i,j,bi,bj)*deepFac2F(ks) |
202 |
jmc |
1.81 |
& /deltaTMom/deltaTFreeSurf |
203 |
jmc |
1.28 |
& *( etaN(i,j,bi,bj) |
204 |
jmc |
1.59 |
& +phi_nh(i,j,ks,bi,bj)*recip_Bo(i,j,bi,bj) ) |
205 |
jmc |
1.51 |
ENDIF |
206 |
jmc |
1.28 |
ENDDO |
207 |
adcroft |
1.12 |
ENDDO |
208 |
jmc |
1.28 |
ELSEIF ( exactConserv ) THEN |
209 |
adcroft |
1.13 |
#else |
210 |
jmc |
1.73 |
C-- Add source term arising from w=d/dt (p_s) |
211 |
jmc |
1.26 |
IF ( exactConserv ) THEN |
212 |
edhill |
1.39 |
#endif /* ALLOW_NONHYDROSTATIC */ |
213 |
jmc |
1.26 |
DO j=1,sNy |
214 |
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DO i=1,sNx |
215 |
jmc |
1.77 |
ks = kSurfC(i,j,bi,bj) |
216 |
jmc |
1.26 |
cg2d_b(i,j,bi,bj) = cg2d_b(i,j,bi,bj) |
217 |
jmc |
1.58 |
& -freeSurfFac*_rA(i,j,bi,bj)*deepFac2F(ks) |
218 |
jmc |
1.81 |
& /deltaTMom/deltaTFreeSurf |
219 |
jmc |
1.26 |
& * etaH(i,j,bi,bj) |
220 |
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ENDDO |
221 |
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ENDDO |
222 |
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ELSE |
223 |
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DO j=1,sNy |
224 |
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DO i=1,sNx |
225 |
jmc |
1.77 |
ks = kSurfC(i,j,bi,bj) |
226 |
jmc |
1.26 |
cg2d_b(i,j,bi,bj) = cg2d_b(i,j,bi,bj) |
227 |
jmc |
1.58 |
& -freeSurfFac*_rA(i,j,bi,bj)*deepFac2F(ks) |
228 |
jmc |
1.81 |
& /deltaTMom/deltaTFreeSurf |
229 |
jmc |
1.26 |
& * etaN(i,j,bi,bj) |
230 |
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ENDDO |
231 |
adcroft |
1.12 |
ENDDO |
232 |
jmc |
1.26 |
ENDIF |
233 |
adcroft |
1.12 |
|
234 |
|
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#ifdef ALLOW_OBCS |
235 |
jmc |
1.76 |
C- Note: solver matrix is trivial outside OB region (main diagonal only) |
236 |
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C => no real need to reset RHS (=cg2d_b) & cg2d_x, except that: |
237 |
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C a) normalisation is fct of Max(RHS), which can be large ouside OB region |
238 |
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C (would be different if we were solving for increment of eta/g |
239 |
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C instead of directly for eta/g). |
240 |
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C => need to reset RHS to ensure that interior solution does not depend |
241 |
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C on ouside OB region. |
242 |
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C b) provide directly the trivial solution cg2d_x == 0 for outside OB region |
243 |
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C (=> no residual => no effect on solver convergence and interior solution) |
244 |
adcroft |
1.14 |
IF (useOBCS) THEN |
245 |
jmc |
1.76 |
DO j=1,sNy |
246 |
|
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DO i=1,sNx |
247 |
|
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cg2d_b(i,j,bi,bj) = cg2d_b(i,j,bi,bj)*maskInC(i,j,bi,bj) |
248 |
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cg2d_x(i,j,bi,bj) = cg2d_x(i,j,bi,bj)*maskInC(i,j,bi,bj) |
249 |
adcroft |
1.12 |
ENDDO |
250 |
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ENDDO |
251 |
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ENDIF |
252 |
jmc |
1.49 |
#endif /* ALLOW_OBCS */ |
253 |
|
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C- end bi,bj loops |
254 |
adcroft |
1.12 |
ENDDO |
255 |
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ENDDO |
256 |
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|
257 |
edhill |
1.42 |
#ifdef ALLOW_DEBUG |
258 |
jmc |
1.77 |
IF ( debugLevel .GE. debLevD ) THEN |
259 |
adcroft |
1.23 |
CALL DEBUG_STATS_RL(1,cg2d_b,'cg2d_b (SOLVE_FOR_PRESSURE)', |
260 |
|
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& myThid) |
261 |
adcroft |
1.24 |
ENDIF |
262 |
adcroft |
1.23 |
#endif |
263 |
jmc |
1.61 |
IF ( DIFFERENT_MULTIPLE(diagFreq, myTime, deltaTClock) ) THEN |
264 |
jmc |
1.83 |
CALL WRITE_FLD_XY_RL( 'cg2d_b', 'I10', cg2d_b, myIter, myThid ) |
265 |
jmc |
1.61 |
ENDIF |
266 |
adcroft |
1.12 |
|
267 |
cnh |
1.1 |
C-- Find the surface pressure using a two-dimensional conjugate |
268 |
jmc |
1.81 |
C gradient solver. See CG2D.h for the interface to this routine. |
269 |
|
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C In rare cases of a poor solver convergence, better to select the |
270 |
|
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C solver minimum-residual solution (instead of the last-iter solution) |
271 |
|
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C by setting cg2dUseMinResSol=1 (<-> nIterMin=0 in input) |
272 |
jmc |
1.79 |
numIters = cg2dMaxIters |
273 |
jmc |
1.81 |
nIterMin = cg2dUseMinResSol - 1 |
274 |
jmc |
1.50 |
c CALL TIMER_START('CG2D [SOLVE_FOR_PRESSURE]',myThid) |
275 |
jmc |
1.80 |
#ifdef DISCONNECTED_TILES |
276 |
|
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C-- Call the not-self-adjoint version of cg2d |
277 |
|
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CALL CG2D_EX0( |
278 |
|
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U cg2d_b, cg2d_x, |
279 |
|
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O firstResidual, minResidualSq, lastResidual, |
280 |
|
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U numIters, nIterMin, |
281 |
|
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I myThid ) |
282 |
|
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#else /* not DISCONNECTED_TILES = default */ |
283 |
heimbach |
1.56 |
#ifdef ALLOW_CG2D_NSA |
284 |
|
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C-- Call the not-self-adjoint version of cg2d |
285 |
|
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CALL CG2D_NSA( |
286 |
jmc |
1.79 |
U cg2d_b, cg2d_x, |
287 |
|
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O firstResidual, minResidualSq, lastResidual, |
288 |
|
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U numIters, nIterMin, |
289 |
heimbach |
1.56 |
I myThid ) |
290 |
|
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#else /* not ALLOW_CG2D_NSA = default */ |
291 |
mlosch |
1.69 |
#ifdef ALLOW_SRCG |
292 |
|
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IF ( useSRCGSolver ) THEN |
293 |
|
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C-- Call the single reduce CG solver |
294 |
|
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CALL CG2D_SR( |
295 |
jmc |
1.79 |
U cg2d_b, cg2d_x, |
296 |
|
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O firstResidual, minResidualSq, lastResidual, |
297 |
|
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U numIters, nIterMin, |
298 |
cnh |
1.1 |
I myThid ) |
299 |
mlosch |
1.69 |
ELSE |
300 |
|
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#else |
301 |
|
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IF (.TRUE.) THEN |
302 |
|
|
C-- Call the default CG solver |
303 |
|
|
#endif /* ALLOW_SRCG */ |
304 |
|
|
CALL CG2D( |
305 |
jmc |
1.79 |
U cg2d_b, cg2d_x, |
306 |
|
|
O firstResidual, minResidualSq, lastResidual, |
307 |
|
|
U numIters, nIterMin, |
308 |
mlosch |
1.69 |
I myThid ) |
309 |
|
|
ENDIF |
310 |
heimbach |
1.56 |
#endif /* ALLOW_CG2D_NSA */ |
311 |
jmc |
1.80 |
#endif /* DISCONNECTED_TILES */ |
312 |
jmc |
1.67 |
_EXCH_XY_RL( cg2d_x, myThid ) |
313 |
jmc |
1.50 |
c CALL TIMER_STOP ('CG2D [SOLVE_FOR_PRESSURE]',myThid) |
314 |
adcroft |
1.23 |
|
315 |
edhill |
1.42 |
#ifdef ALLOW_DEBUG |
316 |
jmc |
1.77 |
IF ( debugLevel .GE. debLevD ) THEN |
317 |
adcroft |
1.23 |
CALL DEBUG_STATS_RL(1,cg2d_x,'cg2d_x (SOLVE_FOR_PRESSURE)', |
318 |
|
|
& myThid) |
319 |
adcroft |
1.24 |
ENDIF |
320 |
adcroft |
1.23 |
#endif |
321 |
cnh |
1.1 |
|
322 |
jmc |
1.32 |
C- dump CG2D output at monitorFreq (to reduce size of STD-OUTPUT files) : |
323 |
jmc |
1.46 |
IF ( DIFFERENT_MULTIPLE(monitorFreq,myTime,deltaTClock) |
324 |
jmc |
1.45 |
& ) THEN |
325 |
heimbach |
1.38 |
IF ( debugLevel .GE. debLevA ) THEN |
326 |
|
|
_BEGIN_MASTER( myThid ) |
327 |
jmc |
1.79 |
WRITE(msgBuf,'(A20,1PE23.14)') 'cg2d_init_res =',firstResidual |
328 |
heimbach |
1.38 |
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
329 |
jmc |
1.79 |
WRITE(msgBuf,'(A27,2I8)') |
330 |
|
|
& 'cg2d_iters(min,last) =', nIterMin, numIters |
331 |
heimbach |
1.38 |
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
332 |
jmc |
1.79 |
IF ( minResidualSq.GE.0. ) THEN |
333 |
|
|
minResidualSq = SQRT(minResidualSq) |
334 |
|
|
WRITE(msgBuf,'(A20,1PE23.14)') 'cg2d_min_res =',minResidualSq |
335 |
|
|
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
336 |
|
|
ENDIF |
337 |
|
|
WRITE(msgBuf,'(A20,1PE23.14)') 'cg2d_last_res =',lastResidual |
338 |
heimbach |
1.38 |
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
339 |
edhill |
1.43 |
_END_MASTER( myThid ) |
340 |
heimbach |
1.38 |
ENDIF |
341 |
jmc |
1.32 |
ENDIF |
342 |
jmc |
1.17 |
|
343 |
jmc |
1.82 |
#ifdef ALLOW_DIAGNOSTICS |
344 |
|
|
C-- Fill diagnostics |
345 |
|
|
IF ( useDiagnostics .AND. implicSurfPress.NE.oneRL ) THEN |
346 |
|
|
diagName = 'PHI_SURF' |
347 |
|
|
IF ( DIAGNOSTICS_IS_ON(diagName,myThid) ) THEN |
348 |
|
|
DO bj=myByLo(myThid),myByHi(myThid) |
349 |
|
|
DO bi=myBxLo(myThid),myBxHi(myThid) |
350 |
|
|
DO j=1-OLy,sNy+OLy |
351 |
|
|
DO i=1-OLx,sNx+OLx |
352 |
|
|
tmpVar(i,j) = implicSurfPress * cg2d_x(i,j,bi,bj) |
353 |
|
|
& + (oneRL - implicSurfPress)* Bo_surf(i,j,bi,bj) |
354 |
|
|
& * etaN(i,j,bi,bj) |
355 |
|
|
ENDDO |
356 |
|
|
ENDDO |
357 |
|
|
CALL DIAGNOSTICS_FILL( tmpVar,diagName,1,1,2,bi,bj,myThid ) |
358 |
|
|
ENDDO |
359 |
|
|
ENDDO |
360 |
|
|
ENDIF |
361 |
|
|
ELSEIF ( useDiagnostics ) THEN |
362 |
|
|
CALL DIAGNOSTICS_FILL( cg2d_x,'PHI_SURF', 0,1, 0,1,1, myThid ) |
363 |
|
|
ENDIF |
364 |
|
|
#endif /* ALLOW_DIAGNOSTICS */ |
365 |
|
|
|
366 |
jmc |
1.17 |
C-- Transfert the 2D-solution to "etaN" : |
367 |
|
|
DO bj=myByLo(myThid),myByHi(myThid) |
368 |
|
|
DO bi=myBxLo(myThid),myBxHi(myThid) |
369 |
|
|
DO j=1-OLy,sNy+OLy |
370 |
|
|
DO i=1-OLx,sNx+OLx |
371 |
jmc |
1.18 |
etaN(i,j,bi,bj) = recip_Bo(i,j,bi,bj)*cg2d_x(i,j,bi,bj) |
372 |
jmc |
1.17 |
ENDDO |
373 |
|
|
ENDDO |
374 |
|
|
ENDDO |
375 |
|
|
ENDDO |
376 |
adcroft |
1.10 |
|
377 |
adcroft |
1.9 |
#ifdef ALLOW_NONHYDROSTATIC |
378 |
jmc |
1.53 |
IF ( use3Dsolver ) THEN |
379 |
jmc |
1.67 |
IF ( DIFFERENT_MULTIPLE(diagFreq, myTime, deltaTClock) ) THEN |
380 |
jmc |
1.83 |
CALL WRITE_FLD_XY_RL( 'cg2d_x','I10', cg2d_x, myIter, myThid ) |
381 |
jmc |
1.67 |
ENDIF |
382 |
adcroft |
1.9 |
|
383 |
|
|
C-- Solve for a three-dimensional pressure term (NH or IGW or both ). |
384 |
|
|
C see CG3D.h for the interface to this routine. |
385 |
jmc |
1.71 |
|
386 |
jmc |
1.73 |
C-- Finish updating cg3d_b: 1) Add EmPmR contribution to top level cg3d_b: |
387 |
|
|
C 2) Update or Add free-surface contribution |
388 |
|
|
C 3) increment in horiz velocity due to new cg2d_x |
389 |
|
|
C 4) add vertical velocity contribution. |
390 |
|
|
CALL PRE_CG3D( |
391 |
|
|
I oldFreeSurfTerm, |
392 |
|
|
I cg2d_x, |
393 |
|
|
U cg3d_b, |
394 |
|
|
I myTime, myIter, myThid ) |
395 |
adcroft |
1.9 |
|
396 |
jmc |
1.67 |
#ifdef ALLOW_DEBUG |
397 |
jmc |
1.77 |
IF ( debugLevel .GE. debLevD ) THEN |
398 |
jmc |
1.73 |
CALL DEBUG_STATS_RL(Nr,cg3d_b,'cg3d_b (SOLVE_FOR_PRESSURE)', |
399 |
|
|
& myThid) |
400 |
|
|
ENDIF |
401 |
jmc |
1.67 |
#endif |
402 |
|
|
IF ( DIFFERENT_MULTIPLE( diagFreq, myTime, deltaTClock) ) THEN |
403 |
jmc |
1.83 |
CALL WRITE_FLD_XYZ_RL('cg3d_b','I10', cg3d_b, myIter,myThid ) |
404 |
jmc |
1.67 |
ENDIF |
405 |
jmc |
1.49 |
|
406 |
jmc |
1.73 |
firstResidual=0. |
407 |
|
|
lastResidual=0. |
408 |
|
|
numIters=cg3dMaxIters |
409 |
|
|
CALL TIMER_START('CG3D [SOLVE_FOR_PRESSURE]',myThid) |
410 |
jmc |
1.80 |
#ifdef DISCONNECTED_TILES |
411 |
|
|
CALL CG3D_EX0( |
412 |
|
|
U cg3d_b, phi_nh, |
413 |
|
|
O firstResidual, lastResidual, |
414 |
|
|
U numIters, |
415 |
|
|
I myIter, myThid ) |
416 |
|
|
#else /* not DISCONNECTED_TILES = default */ |
417 |
jmc |
1.73 |
CALL CG3D( |
418 |
jmc |
1.79 |
U cg3d_b, phi_nh, |
419 |
|
|
O firstResidual, lastResidual, |
420 |
jmc |
1.73 |
U numIters, |
421 |
|
|
I myIter, myThid ) |
422 |
jmc |
1.80 |
#endif /* DISCONNECTED_TILES */ |
423 |
jmc |
1.73 |
_EXCH_XYZ_RL( phi_nh, myThid ) |
424 |
|
|
CALL TIMER_STOP ('CG3D [SOLVE_FOR_PRESSURE]',myThid) |
425 |
|
|
|
426 |
|
|
IF ( DIFFERENT_MULTIPLE(monitorFreq,myTime,deltaTClock) |
427 |
|
|
& ) THEN |
428 |
|
|
IF ( debugLevel .GE. debLevA ) THEN |
429 |
|
|
_BEGIN_MASTER( myThid ) |
430 |
jmc |
1.79 |
WRITE(msgBuf,'(A20,1PE23.14)') 'cg3d_init_res =',firstResidual |
431 |
jmc |
1.73 |
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
432 |
jmc |
1.79 |
WRITE(msgBuf,'(A27,I16)') 'cg3d_iters (last) = ',numIters |
433 |
jmc |
1.73 |
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
434 |
jmc |
1.79 |
WRITE(msgBuf,'(A20,1PE23.14)') 'cg3d_last_res =',lastResidual |
435 |
jmc |
1.73 |
CALL PRINT_MESSAGE(msgBuf,standardMessageUnit,SQUEEZE_RIGHT,1) |
436 |
|
|
_END_MASTER( myThid ) |
437 |
|
|
ENDIF |
438 |
|
|
ENDIF |
439 |
jmc |
1.49 |
|
440 |
jmc |
1.73 |
C-- Separate the Hydrostatic Surface Pressure adjusment (=> put it in dPhiNH) |
441 |
|
|
C from the Non-hydrostatic pressure (since cg3d_x contains both contribution) |
442 |
|
|
IF ( nonHydrostatic .AND. exactConserv ) THEN |
443 |
|
|
IF ( DIFFERENT_MULTIPLE( diagFreq, myTime, deltaTClock) ) THEN |
444 |
jmc |
1.83 |
CALL WRITE_FLD_XYZ_RL('cg3d_x','I10', phi_nh, myIter,myThid ) |
445 |
jmc |
1.73 |
ENDIF |
446 |
|
|
CALL POST_CG3D( |
447 |
|
|
I zeroPsNH, zeroMeanPnh, |
448 |
|
|
I myTime, myIter, myThid ) |
449 |
|
|
ENDIF |
450 |
jmc |
1.49 |
|
451 |
|
|
ENDIF |
452 |
|
|
#endif /* ALLOW_NONHYDROSTATIC */ |
453 |
cnh |
1.1 |
|
454 |
heimbach |
1.60 |
#ifdef ALLOW_SHOWFLOPS |
455 |
|
|
CALL SHOWFLOPS_INSOLVE( myThid) |
456 |
ce107 |
1.52 |
#endif |
457 |
heimbach |
1.60 |
|
458 |
cnh |
1.1 |
RETURN |
459 |
|
|
END |