--- MITgcm/pkg/seaice/seaice_jfnk.F 2013/04/04 07:02:51 1.21 +++ MITgcm/pkg/seaice/seaice_jfnk.F 2013/05/30 14:07:19 1.23 @@ -1,4 +1,4 @@ -C $Header: /home/ubuntu/mnt/e9_copy/MITgcm/pkg/seaice/seaice_jfnk.F,v 1.21 2013/04/04 07:02:51 mlosch Exp $ +C $Header: /home/ubuntu/mnt/e9_copy/MITgcm/pkg/seaice/seaice_jfnk.F,v 1.23 2013/05/30 14:07:19 mlosch Exp $ C $Name: $ #include "SEAICE_OPTIONS.h" @@ -73,10 +73,12 @@ _RL JFNKresidual _RL JFNKresidualKm1 C parameters to compute convergence criterion - _RL phi_e, alp_e, JFNKgamma_lin + _RL JFNKgamma_lin _RL FGMRESeps _RL JFNKtol - +C Adams-Bashforth extrapolation factors + _RL abFac, abAlpha +C _RL recip_deltaT LOGICAL JFNKconverged, krylovConverged LOGICAL writeNow @@ -85,6 +87,9 @@ C u/vIceRes :: residual of sea-ice momentum equations _RL uIceRes(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) _RL vIceRes(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) +C extra time level required for Adams-Bashforth-2 time stepping + _RL duIcNm1(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) + _RL dvIcNm1(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) C du/vIce :: ice velocity increment to be added to u/vIce _RL duIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) _RL dvIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) @@ -113,6 +118,17 @@ & DIFFERENT_MULTIPLE( SEAICE_monFreq, myTime, deltaTClock ) ) & iOutFGMRES=1 +C Adams-Bashforth extrapolation factors + abFac = 0. _d 0 + IF ( SEAICEuseAB2 ) THEN + IF ( myIter.EQ.nIter0 .AND. SEAICEmomStartAB.EQ.0 ) THEN + abFac = 0. _d 0 + ELSE + abFac = 0.5 _d 0 + SEAICE_abEps + ENDIF + ENDIF + abAlpha = 1. _d 0 + abFac + DO bj=myByLo(myThid),myByHi(myThid) DO bi=myBxLo(myThid),myBxHi(myThid) DO J=1-OLy,sNy+OLy @@ -121,21 +137,32 @@ vIceRes(I,J,bi,bj) = 0. _d 0 duIce (I,J,bi,bj) = 0. _d 0 dvIce (I,J,bi,bj) = 0. _d 0 + ENDDO + ENDDO +C cycle ice velocities + DO J=1-OLy,sNy+OLy + DO I=1-OLx,sNx+OLx + duIcNm1(I,J,bi,bj) = uIce(I,J,bi,bj) * abAlpha + & + ( uIce(I,J,bi,bj) - uIceNm1(I,J,bi,bj) ) * abFac + dvIcNm1(I,J,bi,bj) = vIce(I,J,bi,bj) * abAlpha + & + ( vIce(I,J,bi,bj) - vIceNm1(I,J,bi,bj) ) * abFac uIceNm1(I,J,bi,bj) = uIce(I,J,bi,bj) vIceNm1(I,J,bi,bj) = vIce(I,J,bi,bj) ENDDO ENDDO + IF ( .NOT.SEAICEuseIMEX ) THEN C Compute things that do no change during the Newton iteration: C sea-surface tilt and wind stress: -C FORCEX/Y0 - mass*(u/vIceNm1)/deltaT +C FORCEX/Y0 - mass*(abA*u/vIceNm1+abB*(u/vIceNm1-u/vIceNm2))/deltaT DO J=1-OLy,sNy+OLy DO I=1-OLx,sNx+OLx FORCEX(I,J,bi,bj) = FORCEX0(I,J,bi,bj) - & + seaiceMassU(I,J,bi,bj)*uIceNm1(I,J,bi,bj)*recip_deltaT + & + seaiceMassU(I,J,bi,bj)*duIcNm1(I,J,bi,bj)*recip_deltaT FORCEY(I,J,bi,bj) = FORCEY0(I,J,bi,bj) - & + seaiceMassV(I,J,bi,bj)*vIceNm1(I,J,bi,bj)*recip_deltaT + & + seaiceMassV(I,J,bi,bj)*dvIcNm1(I,J,bi,bj)*recip_deltaT ENDDO ENDDO + ENDIF ENDDO ENDDO C Start nonlinear Newton iteration: outer loop iteration @@ -167,10 +194,9 @@ JFNKgamma_lin = JFNKgamma_lin_max IF ( newtonIter.GT.1.AND.newtonIter.LE.SEAICE_JFNK_tolIter & .AND.JFNKresidual.LT.JFNKres_t ) THEN -C Eisenstat, 1996, equ.(2.6) - phi_e = 1. _d 0 - alp_e = 1. _d 0 - JFNKgamma_lin = phi_e*( JFNKresidual/JFNKresidualKm1 )**alp_e +C Eisenstat and Walker (1996), eq.(2.6) + JFNKgamma_lin = SEAICE_JFNKphi + & *( JFNKresidual/JFNKresidualKm1 )**SEAICE_JFNKalpha JFNKgamma_lin = min(JFNKgamma_lin_max, JFNKgamma_lin) JFNKgamma_lin = max(JFNKgamma_lin_min, JFNKgamma_lin) ENDIF