C $Header: /home/ubuntu/mnt/e9_copy/MITgcm/pkg/seaice/seaice_calc_residual.F,v 1.1 2012/10/16 07:00:21 mlosch Exp $ C $Name: $ #include "SEAICE_OPTIONS.h" CBOP C !ROUTINE: SEAICE_CALC_RESIDUAL C !INTERFACE: SUBROUTINE SEAICE_CALC_RESIDUAL( I uIceLoc, vIceLoc, O uIceRes, vIceRes, I newtonIter, krylovIter, myTime, myIter, myThid ) C !DESCRIPTION: \bv C *==========================================================* C | SUBROUTINE SEAICE_CALC_RESIDUAL C | o For Jacobian-free Newton-Krylov solver compute C | the residual of the momentum equations C *==========================================================* C | written by Martin Losch, Oct 2012 C *==========================================================* C \ev C !USES: IMPLICIT NONE C === Global variables === #include "SIZE.h" #include "EEPARAMS.h" #include "PARAMS.h" #include "DYNVARS.h" #include "GRID.h" #include "SEAICE_SIZE.h" #include "SEAICE_PARAMS.h" #include "SEAICE.h" C !INPUT/OUTPUT PARAMETERS: C === Routine arguments === C myTime :: Simulation time C myIter :: Simulation timestep number C myThid :: my Thread Id. number C newtonIter :: current iterate of Newton iteration C krylovIter :: current iterate of Krylov iteration _RL myTime INTEGER myIter INTEGER myThid INTEGER newtonIter INTEGER krylovIter C u/vIceLoc :: local copies of the current ice velocity _RL uIceLoc(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) _RL vIceLoc(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) 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) #if ( (defined SEAICE_CGRID) && \ (defined SEAICE_ALLOW_JFNK) && \ (defined SEAICE_ALLOW_DYNAMICS) ) C u/vIceLHS :: left hand side of momentum equations _RL uIceLHS(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) _RL vIceLHS(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) C u/vIceRHS :: righ hand side of momentum equations _RL uIceRHS(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) _RL vIceRHS(1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) C i,j,bi,bj :: loop indices INTEGER i,j,bi,bj CEOP C Initialise DO bj=myByLo(myThid),myByHi(myThid) DO bi=myBxLo(myThid),myBxHi(myThid) DO J=1-Oly,sNy+Oly DO I=1-Olx,sNx+Olx uIceLHS(I,J,bi,bj) = 0. _d 0 vIceLHS(I,J,bi,bj) = 0. _d 0 uIceRHS(I,J,bi,bj) = 0. _d 0 vIceRHS(I,J,bi,bj) = 0. _d 0 ENDDO ENDDO ENDDO ENDDO C u/vIceLoc have changed so that new drag coefficients and C viscosities are required CALL SEAICE_OCEANDRAG_COEFFS( I uIceLoc, vIceLoc, O DWATN, I krylovIter, myTime, myIter, myThid ) CALL SEAICE_CALC_STRAINRATES( I uIceLoc, vIceLoc, O e11, e22, e12, I krylovIter, myTime, myIter, myThid ) CALL SEAICE_CALC_VISCOSITIES( I e11, e22, e12, zMin, zMax, hEffM, press0, O eta, zeta, press, I krylovIter, myTime, myIter, myThid ) C The scheme is backward Euler in time, i.e. the rhs-vector contains C only terms that are independent of u/vIce, except for the time C derivative part mass*(u/vIce-u/vIceNm1)/deltaT C compute new right hand side (depends to DWATN=Cdrag) C sea-surface tilt and wind stress: FORCEX0, FORCEY0 C + mass*(u/vIceNm1)/deltaT C + Cdrag*(uVel*cosWat - vVel*sinWat)/(vVel*cosWat + uVel*sinWat) CALL SEAICE_CALC_RHS( O uIceRHS, vIceRHS, I newtonIter, krylovIter, myTime, myIter, myThid ) C Left-hand side contributions: C + mass*(u/vIce)/deltaT C + Cdrag*(uIce*cosWat - vIce*sinWat)/(vIce*cosWat + uIce*sinWat) C - mass*f*vIce/+mass*f*uIce C - dsigma/dx / -dsigma/dy, eta and zeta are only computed once per C Newton iterate CALL SEAICE_CALC_LHS( I uIceLoc, vIceLoc, O uIceLHS, vIceLHS, I newtonIter, myTime, myIter, myThid ) C Right-hand side contributions only need to be computed once per C time step, therefore we will put them into a separate routine C and call them elsewhere to save floating point operations C Calculate the residual DO bj=myByLo(myThid),myByHi(myThid) DO bi=myBxLo(myThid),myBxHi(myThid) DO J=1,sNy DO I=1,sNx uIceRes(I,J,bi,bj) = uIceLHS(I,J,bi,bj) - uIceRHS(I,J,bi,bj) vIceRes(I,J,bi,bj) = vIceLHS(I,J,bi,bj) - vIceRHS(I,J,bi,bj) ENDDO ENDDO ENDDO ENDDO #endif /* SEAICE_ALLOW_DYNAMICS and SEAICE_CGRID and SEAICE_ALLOW_JFNK */ RETURN END