3 |
|
|
4 |
#include "SEAICE_OPTIONS.h" |
#include "SEAICE_OPTIONS.h" |
5 |
|
|
6 |
|
C-- File seaice_jfnk.F: seaice jfnk dynamical solver S/R: |
7 |
|
C-- Contents |
8 |
|
C-- o SEAICE_JFNK |
9 |
|
C-- o SEAICE_JFNK_UPDATE |
10 |
|
|
11 |
CBOP |
CBOP |
12 |
C !ROUTINE: SEAICE_JFNK |
C !ROUTINE: SEAICE_JFNK |
13 |
C !INTERFACE: |
C !INTERFACE: |
15 |
|
|
16 |
C !DESCRIPTION: \bv |
C !DESCRIPTION: \bv |
17 |
C *==========================================================* |
C *==========================================================* |
18 |
C | SUBROUTINE SEAICE_JFKF |
C | SUBROUTINE SEAICE_JFNK |
19 |
C | o Ice dynamics using a Jacobian-free Newton-Krylov solver |
C | o Ice dynamics using a Jacobian-free Newton-Krylov solver |
20 |
C | following J.-F. Lemieux et al. Improving the numerical |
C | following J.-F. Lemieux et al. Improving the numerical |
21 |
C | convergence of viscous-plastic sea ice models with the |
C | convergence of viscous-plastic sea ice models with the |
60 |
LOGICAL DIFFERENT_MULTIPLE |
LOGICAL DIFFERENT_MULTIPLE |
61 |
EXTERNAL DIFFERENT_MULTIPLE |
EXTERNAL DIFFERENT_MULTIPLE |
62 |
|
|
63 |
|
C !LOCAL VARIABLES: |
64 |
|
C === Local variables === |
65 |
C i,j,bi,bj :: loop indices |
C i,j,bi,bj :: loop indices |
66 |
INTEGER i,j,bi,bj |
INTEGER i,j,bi,bj |
67 |
C loop indices |
C loop indices |
68 |
INTEGER newtonIter |
INTEGER newtonIter |
69 |
INTEGER krylovIter, krylovFails |
INTEGER krylovIter, krylovFails |
70 |
INTEGER totalKrylovItersLoc |
INTEGER totalKrylovItersLoc, totalNewtonItersLoc |
71 |
C FGMRES flag that determines amount of output messages of fgmres |
C FGMRES flag that determines amount of output messages of fgmres |
72 |
INTEGER iOutFGMRES |
INTEGER iOutFGMRES |
73 |
C FGMRES flag that indicates what fgmres wants us to do next |
C FGMRES flag that indicates what fgmres wants us to do next |
74 |
INTEGER iCode |
INTEGER iCode |
75 |
_RL JFNKresidual, JFNKresidualTile(nSx,nSy) |
_RL JFNKresidual |
76 |
_RL JFNKresidualKm1 |
_RL JFNKresidualKm1 |
77 |
C parameters to compute convergence criterion |
C parameters to compute convergence criterion |
78 |
_RL phi_e, alp_e, JFNKgamma_lin |
_RL phi_e, alp_e, JFNKgamma_lin |
87 |
C u/vIceRes :: residual of sea-ice momentum equations |
C u/vIceRes :: residual of sea-ice momentum equations |
88 |
_RL uIceRes(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
_RL uIceRes(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
89 |
_RL vIceRes(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
_RL vIceRes(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
90 |
|
C vector version of the residuals |
91 |
|
_RL resTmp (nVec,1,nSx,nSy) |
92 |
C du/vIce :: ice velocity increment to be added to u/vIce |
C du/vIce :: ice velocity increment to be added to u/vIce |
93 |
_RL duIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
_RL duIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
94 |
_RL dvIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
_RL dvIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
98 |
_RL etaPre (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
_RL etaPre (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
99 |
_RL etaZPre (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
_RL etaZPre (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
100 |
_RL dwatPre (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
_RL dwatPre (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
|
_RL pressPre(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
|
101 |
CEOP |
CEOP |
102 |
|
|
103 |
C Initialise |
C Initialise |
112 |
recip_deltaT = 1. _d 0 / SEAICE_deltaTdyn |
recip_deltaT = 1. _d 0 / SEAICE_deltaTdyn |
113 |
|
|
114 |
iOutFGMRES=0 |
iOutFGMRES=0 |
115 |
C iOutFgmres=1 gives a little bit of output |
C with iOutFgmres=1, seaice_fgmres prints the residual at each iteration |
116 |
IF ( debugLevel.GE.debLevA .AND. |
IF ( debugLevel.GE.debLevC .AND. |
117 |
& DIFFERENT_MULTIPLE( SEAICE_monFreq, myTime, deltaTClock ) ) |
& DIFFERENT_MULTIPLE( SEAICE_monFreq, myTime, deltaTClock ) ) |
118 |
& iOutFGMRES=1 |
& iOutFGMRES=1 |
119 |
|
|
149 |
newtonIter = newtonIter + 1 |
newtonIter = newtonIter + 1 |
150 |
C Compute initial residual F(u), (includes computation of global |
C Compute initial residual F(u), (includes computation of global |
151 |
C variables DWATN, zeta, and eta) |
C variables DWATN, zeta, and eta) |
152 |
CALL SEAICE_CALC_RESIDUAL( |
IF ( newtonIter .EQ. 1 ) CALL SEAICE_JFNK_UPDATE( |
153 |
I uIce, vIce, |
I duIce, dvIce, |
154 |
O uIceRes, vIceRes, |
U uIce, vIce, JFNKresidual, |
155 |
I newtonIter, 0, myTime, myIter, myThid ) |
O uIceRes, vIceRes, |
156 |
CALL EXCH_UV_XY_RL( uIceRes, vIceRes,.TRUE.,myThid) |
I newtonIter, myTime, myIter, myThid ) |
157 |
C local copies of precomputed coefficients that are to stay |
C local copies of precomputed coefficients that are to stay |
158 |
C constant for the preconditioner |
C constant for the preconditioner |
159 |
DO bj=myByLo(myThid),myByHi(myThid) |
DO bj=myByLo(myThid),myByHi(myThid) |
160 |
DO bi=myBxLo(myThid),myBxHi(myThid) |
DO bi=myBxLo(myThid),myBxHi(myThid) |
161 |
DO j=1-Oly,sNy+Oly |
DO j=1-Oly,sNy+Oly |
162 |
DO i=1-Olx,sNx+Olx |
DO i=1-Olx,sNx+Olx |
163 |
zetaPre(I,J,bi,bj) = zeta(I,J,bi,bj) |
zetaPre(I,J,bi,bj) = zeta(I,J,bi,bj) |
164 |
etaPre(I,J,bi,bj) = eta(I,J,bi,bj) |
etaPre(I,J,bi,bj) = eta(I,J,bi,bj) |
165 |
etaZPre(I,J,bi,bj) = etaZ(I,J,bi,bj) |
etaZPre(I,J,bi,bj) = etaZ(I,J,bi,bj) |
166 |
dwatPre(I,J,bi,bj) = DWATN(I,J,bi,bj) |
dwatPre(I,J,bi,bj) = DWATN(I,J,bi,bj) |
|
pressPre(I,J,bi,bj) = press(I,J,bi,bj) |
|
|
ENDDO |
|
|
ENDDO |
|
|
ENDDO |
|
|
ENDDO |
|
|
C |
|
|
DO bj=myByLo(myThid),myByHi(myThid) |
|
|
DO bi=myBxLo(myThid),myBxHi(myThid) |
|
|
JFNKresidualTile(bi,bj) = 0. _d 0 |
|
|
DO J=1,sNy |
|
|
DO I=1,sNx |
|
|
#ifdef CG2D_SINGLECPU_SUM |
|
|
JFNKlocalBuf(I,J,bi,bj) = |
|
|
#else |
|
|
JFNKresidualTile(bi,bj) = JFNKresidualTile(bi,bj) + |
|
|
#endif |
|
|
& uIceRes(I,J,bi,bj)*uIceRes(I,J,bi,bj) + |
|
|
& vIceRes(I,J,bi,bj)*vIceRes(I,J,bi,bj) |
|
167 |
ENDDO |
ENDDO |
168 |
ENDDO |
ENDDO |
169 |
ENDDO |
ENDDO |
170 |
ENDDO |
ENDDO |
|
JFNKresidual = 0. _d 0 |
|
|
#ifdef CG2D_SINGLECPU_SUM |
|
|
CALL GLOBAL_SUM_SINGLECPU_RL( |
|
|
& JFNKlocalBuf,JFNKresidual, 0, 0, myThid) |
|
|
#else |
|
|
CALL GLOBAL_SUM_TILE_RL( JFNKresidualTile,JFNKresidual,myThid ) |
|
|
#endif |
|
|
JFNKresidual = SQRT(JFNKresidual) |
|
171 |
C compute convergence criterion for linear preconditioned FGMRES |
C compute convergence criterion for linear preconditioned FGMRES |
172 |
JFNKgamma_lin = JFNKgamma_lin_max |
JFNKgamma_lin = JFNKgamma_lin_max |
173 |
IF ( newtonIter.GT.1.AND.newtonIter.LE.100 |
IF ( newtonIter.GT.1.AND.newtonIter.LE.100 |
189 |
C in that routine |
C in that routine |
190 |
krylovIter = 0 |
krylovIter = 0 |
191 |
iCode = 0 |
iCode = 0 |
|
IF ( debugLevel.GE.debLevA ) THEN |
|
|
_BEGIN_MASTER( myThid ) |
|
|
WRITE(msgBuf,'(2A,2(1XI6),2E12.5)') |
|
|
& ' S/R SEAICE_JFNK: newtonIter,', |
|
|
& ' total newtonIter, JFNKgamma_lin, initial norm = ', |
|
|
& newtonIter,SEAICEnewtonIterMax*(myIter-nIter0)+newtonIter, |
|
|
& JFNKgamma_lin, JFNKresidual |
|
|
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
|
|
& SQUEEZE_RIGHT, myThid ) |
|
|
_END_MASTER( myThid ) |
|
|
ENDIF |
|
192 |
C |
C |
193 |
JFNKconverged = JFNKresidual.LT.JFNKtol |
JFNKconverged = JFNKresidual.LT.JFNKtol |
194 |
C |
C |
218 |
IF ( SOLV_MAX_ITERS .GT. 0 ) |
IF ( SOLV_MAX_ITERS .GT. 0 ) |
219 |
& CALL SEAICE_PRECONDITIONER( |
& CALL SEAICE_PRECONDITIONER( |
220 |
U duIce, dvIce, |
U duIce, dvIce, |
221 |
I zetaPre, etaPre, etaZpre, dwatPre, pressPre, |
I zetaPre, etaPre, etaZpre, dwatPre, |
222 |
I newtonIter, krylovIter, myTime, myIter, myThid ) |
I newtonIter, krylovIter, myTime, myIter, myThid ) |
223 |
ELSEIF (iCode.GE.2) THEN |
ELSEIF (iCode.GE.2) THEN |
224 |
C Compute Jacobian times vector |
C Compute Jacobian times vector |
234 |
C some output diagnostics |
C some output diagnostics |
235 |
IF ( debugLevel.GE.debLevA ) THEN |
IF ( debugLevel.GE.debLevA ) THEN |
236 |
_BEGIN_MASTER( myThid ) |
_BEGIN_MASTER( myThid ) |
237 |
|
totalNewtonItersLoc = |
238 |
|
& SEAICEnewtonIterMax*(myIter-nIter0)+newtonIter |
239 |
|
WRITE(msgBuf,'(2A,2(1XI6),2E12.5)') |
240 |
|
& ' S/R SEAICE_JFNK: Newton iterate / total, ', |
241 |
|
& 'JFNKgamma_lin, initial norm = ', |
242 |
|
& newtonIter, totalNewtonItersLoc, |
243 |
|
& JFNKgamma_lin,JFNKresidual |
244 |
|
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
245 |
|
& SQUEEZE_RIGHT, myThid ) |
246 |
WRITE(msgBuf,'(3(A,I6))') |
WRITE(msgBuf,'(3(A,I6))') |
247 |
& ' S/R SEAICE_JFNK: Newton iterate / total = ', newtonIter, |
& ' S/R SEAICE_JFNK: Newton iterate / total = ',newtonIter, |
248 |
& ' / ', SEAICEnewtonIterMax*(myIter-nIter0)+newtonIter, |
& ' / ', totalNewtonItersLoc, |
249 |
& ', Nb. of FGMRES iterations = ', krylovIter |
& ', Nb. of FGMRES iterations = ', krylovIter |
250 |
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
251 |
& SQUEEZE_RIGHT, myThid ) |
& SQUEEZE_RIGHT, myThid ) |
254 |
IF ( krylovIter.EQ.SEAICEkrylovIterMax ) THEN |
IF ( krylovIter.EQ.SEAICEkrylovIterMax ) THEN |
255 |
krylovFails = krylovFails + 1 |
krylovFails = krylovFails + 1 |
256 |
ENDIF |
ENDIF |
257 |
|
C Set the stopping criterion for the Newton iteration |
258 |
|
IF ( newtonIter .EQ. 1 ) JFNKtol=JFNKgamma_nonlin*JFNKresidual |
259 |
C Update linear solution vector and return to Newton iteration |
C Update linear solution vector and return to Newton iteration |
260 |
|
C Do a linesearch if necessary, and compute a new residual. |
261 |
|
C Note that it should be possible to do the following operations |
262 |
|
C at the beginning of the Newton iteration, thereby saving us from |
263 |
|
C the extra call of seaice_jfnk_update, but unfortunately that |
264 |
|
C changes the results, so we leave the stuff here for now. |
265 |
|
CALL SEAICE_JFNK_UPDATE( |
266 |
|
I duIce, dvIce, |
267 |
|
U uIce, vIce, JFNKresidual, |
268 |
|
O uIceRes, vIceRes, |
269 |
|
I newtonIter, myTime, myIter, myThid ) |
270 |
|
C reset du/vIce here instead of setting sol = 0 in seaice_fgmres_driver |
271 |
DO bj=myByLo(myThid),myByHi(myThid) |
DO bj=myByLo(myThid),myByHi(myThid) |
272 |
DO bi=myBxLo(myThid),myBxHi(myThid) |
DO bi=myBxLo(myThid),myBxHi(myThid) |
273 |
DO J=1-Oly,sNy+Oly |
DO J=1-Oly,sNy+Oly |
274 |
DO I=1-Olx,sNx+Olx |
DO I=1-Olx,sNx+Olx |
|
uIce(I,J,bi,bj) = uIce(I,J,bi,bj)+duIce(I,J,bi,bj) |
|
|
vIce(I,J,bi,bj) = vIce(I,J,bi,bj)+dvIce(I,J,bi,bj) |
|
|
C reset du/vIce here instead of setting sol = 0 in seaice_fgmres_driver |
|
275 |
duIce(I,J,bi,bj)= 0. _d 0 |
duIce(I,J,bi,bj)= 0. _d 0 |
276 |
dvIce(I,J,bi,bj)= 0. _d 0 |
dvIce(I,J,bi,bj)= 0. _d 0 |
277 |
ENDDO |
ENDDO |
278 |
ENDDO |
ENDDO |
279 |
ENDDO |
ENDDO |
280 |
ENDDO |
ENDDO |
|
C Set the stopping criterion for the Newton iteration |
|
|
IF ( newtonIter .EQ. 1 ) JFNKtol=JFNKgamma_nonlin*JFNKresidual |
|
281 |
ENDIF |
ENDIF |
282 |
C end of Newton iterate |
C end of Newton iterate |
283 |
ENDDO |
ENDDO |
347 |
&' // =======================================================' |
&' // =======================================================' |
348 |
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
349 |
& SQUEEZE_RIGHT, myThid ) |
& SQUEEZE_RIGHT, myThid ) |
350 |
WRITE(msgBuf,'(A)') ' // Begin JFNK statistics' |
WRITE(msgBuf,'(A)') ' // End JFNK statistics' |
351 |
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
352 |
& SQUEEZE_RIGHT, myThid ) |
& SQUEEZE_RIGHT, myThid ) |
353 |
WRITE(msgBuf,'(A)') |
WRITE(msgBuf,'(A)') |
392 |
_END_MASTER( myThid ) |
_END_MASTER( myThid ) |
393 |
ENDIF |
ENDIF |
394 |
|
|
395 |
|
RETURN |
396 |
|
END |
397 |
|
|
398 |
|
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
399 |
|
CBOP |
400 |
|
C !ROUTINE: SEAICE_JFNK_UPDATE |
401 |
|
C !INTERFACE: |
402 |
|
|
403 |
|
SUBROUTINE SEAICE_JFNK_UPDATE( |
404 |
|
I duIce, dvIce, |
405 |
|
U uIce, vIce, JFNKresidual, |
406 |
|
O uIceRes, vIceRes, |
407 |
|
I newtonIter, myTime, myIter, myThid ) |
408 |
|
|
409 |
|
C !DESCRIPTION: \bv |
410 |
|
C *==========================================================* |
411 |
|
C | SUBROUTINE SEAICE_JFNK_UPDATE |
412 |
|
C | o Update velocities with incremental solutions of FGMRES |
413 |
|
C | o compute residual of updated solutions and do |
414 |
|
C | o linesearch: |
415 |
|
C | reduce update until residual is smaller than previous |
416 |
|
C | one (input) |
417 |
|
C *==========================================================* |
418 |
|
C | written by Martin Losch, Jan 2013 |
419 |
|
C *==========================================================* |
420 |
|
C \ev |
421 |
|
|
422 |
|
C !USES: |
423 |
|
IMPLICIT NONE |
424 |
|
|
425 |
|
C === Global variables === |
426 |
|
#include "SIZE.h" |
427 |
|
#include "EEPARAMS.h" |
428 |
|
#include "PARAMS.h" |
429 |
|
#include "SEAICE_SIZE.h" |
430 |
|
#include "SEAICE_PARAMS.h" |
431 |
|
|
432 |
|
C !INPUT/OUTPUT PARAMETERS: |
433 |
|
C === Routine arguments === |
434 |
|
C myTime :: Simulation time |
435 |
|
C myIter :: Simulation timestep number |
436 |
|
C myThid :: my Thread Id. number |
437 |
|
C newtonIter :: current iterate of Newton iteration |
438 |
|
_RL myTime |
439 |
|
INTEGER myIter |
440 |
|
INTEGER myThid |
441 |
|
INTEGER newtonIter |
442 |
|
C JFNKresidual :: Residual at the beginning of the FGMRES iteration, |
443 |
|
C changes with newtonIter (updated) |
444 |
|
_RL JFNKresidual |
445 |
|
C du/vIce :: ice velocity increment to be added to u/vIce (input) |
446 |
|
_RL duIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
447 |
|
_RL dvIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
448 |
|
C u/vIce :: ice velocity increment to be added to u/vIce (updated) |
449 |
|
_RL uIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
450 |
|
_RL vIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
451 |
|
C u/vIceRes :: residual of sea-ice momentum equations (output) |
452 |
|
_RL uIceRes(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
453 |
|
_RL vIceRes(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
454 |
|
|
455 |
|
C !LOCAL VARIABLES: |
456 |
|
C === Local variables === |
457 |
|
C i,j,bi,bj :: loop indices |
458 |
|
INTEGER i,j,bi,bj |
459 |
|
INTEGER l |
460 |
|
_RL resLoc, facLS |
461 |
|
LOGICAL doLineSearch |
462 |
|
C nVec :: size of the input vector(s) |
463 |
|
C vector version of the residuals |
464 |
|
INTEGER nVec |
465 |
|
PARAMETER ( nVec = 2*sNx*sNy ) |
466 |
|
_RL resTmp (nVec,1,nSx,nSy) |
467 |
|
C |
468 |
|
CHARACTER*(MAX_LEN_MBUF) msgBuf |
469 |
|
CEOP |
470 |
|
|
471 |
|
C Initialise some local variables |
472 |
|
l = 0 |
473 |
|
resLoc = JFNKresidual |
474 |
|
facLS = 1. _d 0 |
475 |
|
doLineSearch = .TRUE. |
476 |
|
DO WHILE ( doLineSearch ) |
477 |
|
C Determine, if we need more iterations |
478 |
|
doLineSearch = resLoc .GE. JFNKresidual |
479 |
|
C Limit the maximum number of iterations arbitrarily to four |
480 |
|
doLineSearch = doLineSearch .AND. l .LE. 4 |
481 |
|
C For the first iteration du/vIce = 0 and there will be no |
482 |
|
C improvement of the residual possible, so we do only the first |
483 |
|
C iteration |
484 |
|
IF ( newtonIter .EQ. 1 ) doLineSearch = .FALSE. |
485 |
|
C Only start a linesearch after some Newton iterations |
486 |
|
IF ( newtonIter .LE. SEAICE_JFNK_lsIter ) doLineSearch = .FALSE. |
487 |
|
C Increment counter |
488 |
|
l = l + 1 |
489 |
|
C Create update |
490 |
|
DO bj=myByLo(myThid),myByHi(myThid) |
491 |
|
DO bi=myBxLo(myThid),myBxHi(myThid) |
492 |
|
DO J=1-Oly,sNy+Oly |
493 |
|
DO I=1-Olx,sNx+Olx |
494 |
|
uIce(I,J,bi,bj) = uIce(I,J,bi,bj)+facLS*duIce(I,J,bi,bj) |
495 |
|
vIce(I,J,bi,bj) = vIce(I,J,bi,bj)+facLS*dvIce(I,J,bi,bj) |
496 |
|
ENDDO |
497 |
|
ENDDO |
498 |
|
ENDDO |
499 |
|
ENDDO |
500 |
|
C Compute current residual F(u), (includes re-computation of global |
501 |
|
C variables DWATN, zeta, and eta, i.e. they are different after this) |
502 |
|
CALL SEAICE_CALC_RESIDUAL( |
503 |
|
I uIce, vIce, |
504 |
|
O uIceRes, vIceRes, |
505 |
|
I newtonIter, 0, myTime, myIter, myThid ) |
506 |
|
C Important: Compute the norm of the residual using the same scalar |
507 |
|
C product that SEAICE_FGMRES does |
508 |
|
CALL SEAICE_MAP2VEC(nVec,uIceRes,vIceRes,resTmp,.TRUE.,myThid) |
509 |
|
CALL SEAICE_SCALPROD(nVec,1,1,1,resTmp,resTmp,resLoc,myThid) |
510 |
|
resLoc = SQRT(resLoc) |
511 |
|
C some output diagnostics |
512 |
|
IF ( debugLevel.GE.debLevA .AND. doLineSearch ) THEN |
513 |
|
_BEGIN_MASTER( myThid ) |
514 |
|
WRITE(msgBuf,'(2A,2(1XI6),3E12.5)') |
515 |
|
& ' S/R SEAICE_JFNK_UPDATE: Newton iter, LSiter, ', |
516 |
|
& 'facLS, JFNKresidual, resLoc = ', |
517 |
|
& newtonIter, l, facLS, JFNKresidual, resLoc |
518 |
|
CALL PRINT_MESSAGE( msgBuf, standardMessageUnit, |
519 |
|
& SQUEEZE_RIGHT, myThid ) |
520 |
|
_END_MASTER( myThid ) |
521 |
|
ENDIF |
522 |
|
C Get ready for the next iteration: after adding du/vIce in the first |
523 |
|
C iteration, we substract 0.5*du/vIce from u/vIce in the next |
524 |
|
C iterations, 0.25*du/vIce in the second, etc. |
525 |
|
facLS = - 0.5 _d 0 * ABS(facLS) |
526 |
|
ENDDO |
527 |
|
C This is the new residual |
528 |
|
JFNKresidual = resLoc |
529 |
|
|
530 |
#endif /* SEAICE_ALLOW_DYNAMICS and SEAICE_CGRID and SEAICE_ALLOW_JFNK */ |
#endif /* SEAICE_ALLOW_DYNAMICS and SEAICE_CGRID and SEAICE_ALLOW_JFNK */ |
531 |
|
|
532 |
RETURN |
RETURN |