C $Header: /home/ubuntu/mnt/e9_copy/MITgcm/pkg/seaice/seaice_calc_strainrates.F,v 1.14 2009/06/24 08:23:38 mlosch Exp $ C $Name: $ #include "SEAICE_OPTIONS.h" CStartOfInterface SUBROUTINE SEAICE_CALC_STRAINRATES( I uFld, vFld, O e11Loc, e22Loc, e12Loc, I iStep, myTime, myIter, myThid ) C /==========================================================\ C | SUBROUTINE SEAICE_CALC_STRAINRATES | C | o compute strain rates from ice velocities | C |==========================================================| C | written by Martin Losch, Apr 2007 | C \==========================================================/ IMPLICIT NONE C === Global variables === #include "SIZE.h" #include "EEPARAMS.h" #include "PARAMS.h" #include "GRID.h" #include "SEAICE_PARAMS.h" #include "SEAICE.h" #ifdef ALLOW_AUTODIFF_TAMC # include "tamc.h" #endif C === Routine arguments === C iStep :: Sub-time-step number C myTime :: Simulation time C myIter :: Simulation timestep number C myThid :: My Thread Id. number INTEGER iStep _RL myTime INTEGER myIter INTEGER myThid C ice velocities _RL uFld (1-Olx:sNx+Olx,1-Oly:sNy+Oly,nSx,nSy) _RL vFld (1-Olx:sNx+Olx,1-Oly:sNy+Oly,nSx,nSy) C strain rate tensor _RL e11Loc (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) _RL e22Loc (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) _RL e12Loc (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) CEndOfInterface #ifdef SEAICE_CGRID #ifdef SEAICE_ALLOW_DYNAMICS C === Local variables === C i,j,bi,bj - Loop counters INTEGER i, j, bi, bj C hFacU, hFacV - determine the no-slip boundary condition INTEGER k _RS hFacU, hFacV, noSlipFac k = 1 noSlipFac = 0. _d 0 IF ( SEAICE_no_slip ) noSlipFac = 1. _d 0 C #ifndef SEAICE_OLD_AND_BAD_DISCRETIZATION DO bj=myByLo(myThid),myByHi(myThid) DO bi=myBxLo(myThid),myBxHi(myThid) DO j=1-Oly,sNy+Oly-1 DO i=1-Olx,sNx+Olx-1 C evaluate strain rates e11Loc(I,J,bi,bj) = _recip_dxF(I,J,bi,bj) * & (uFld(I+1,J,bi,bj)-uFld(I,J,bi,bj)) & +HALF* & (vFld(I,J,bi,bj)+vFld(I,J+1,bi,bj)) & * k2AtC(I,J,bi,bj) e22Loc(I,J,bi,bj) = _recip_dyF(I,J,bi,bj) * & (vFld(I,J+1,bi,bj)-vFld(I,J,bi,bj)) & +HALF* & (uFld(I,J,bi,bj)+uFld(I+1,J,bi,bj)) & * k1AtC(I,J,bi,bj) ENDDO ENDDO DO j=1-Oly+1,sNy+Oly DO i=1-Olx+1,sNx+Olx hFacU = _maskW(i,j,k,bi,bj) - _maskW(i,j-1,k,bi,bj) hFacV = _maskS(i,j,k,bi,bj) - _maskS(i-1,j,k,bi,bj) e12Loc(I,J,bi,bj) = HALF*( & ( uFld(I,J,bi,bj) - uFld(I ,J-1,bi,bj) ) & * _recip_dyU(I,J,bi,bj) & + ( vFld(I,J,bi,bj) - vFld(I-1,J ,bi,bj) ) & * _recip_dxV(I,J,bi,bj) & - k1AtZ(I,J,bi,bj) & * 0.5 _d 0 * (vFld(I,J,bi,bj)+vFld(I-1,J ,bi,bj)) & - k2AtZ(I,J,bi,bj) & * 0.5 _d 0 * (uFld(I,J,bi,bj)+uFld(I ,J-1,bi,bj)) & ) & *maskC(I ,J ,k,bi,bj)*maskC(I-1,J ,k,bi,bj) & *maskC(I ,J-1,k,bi,bj)*maskC(I-1,J-1,k,bi,bj) & + 2.0 _d 0 * noSlipFac * ( & ( uFld(I,J,bi,bj) + uFld(I ,J-1,bi,bj) ) & * _recip_dyU(I,J,bi,bj) * hFacU & + ( vFld(I,J,bi,bj) + vFld(I-1,J ,bi,bj) ) & * _recip_dxV(I,J,bi,bj) * hFacV & ) C no slip at the boundary implies u(j)+u(j-1)=0 and v(i)+v(i-1)=0 C accross the boundary; this is already accomplished by masking so C that the following lines are not necessary c$$$ & - hFacV * k1AtZ(I,J,bi,bj) c$$$ & * 0.5 _d 0 * (vFld(I,J,bi,bj)+vFld(I-1,J ,bi,bj)) c$$$ & - hFacU * k2AtZ(I,J,bi,bj) c$$$ & * 0.5 _d 0 * (uFld(I,J,bi,bj)+uFld(I ,J-1,bi,bj)) ENDDO ENDDO c$$$ ENDIF ENDDO ENDDO #else C this the old and incomplete discretization, here I also erroneously C used finite-volumes to discretize the strain rates DO bj=myByLo(myThid),myByHi(myThid) DO bi=myBxLo(myThid),myBxHi(myThid) DO j=1-Oly,sNy+Oly-1 DO i=1-Olx,sNx+Olx-1 C evaluate strain rates e11Loc(I,J,bi,bj) = _recip_dxF(I,J,bi,bj) * & (uFld(I+1,J,bi,bj)-uFld(I,J,bi,bj)) & -HALF* & (vFld(I,J,bi,bj)+vFld(I,J+1,bi,bj)) & * _tanPhiAtU(I,J,bi,bj)*recip_rSphere e22Loc(I,J,bi,bj) = _recip_dyF(I,J,bi,bj) * & (vFld(I,J+1,bi,bj)-vFld(I,J,bi,bj)) C one metric term is missing ENDDO ENDDO DO j=1-Oly+1,sNy+Oly DO i=1-Olx+1,sNx+Olx e12Loc(I,J,bi,bj) = HALF*( & (uFld(I ,J ,bi,bj) * _dxC(I ,J ,bi,bj) & -uFld(I ,J-1,bi,bj) * _dxC(I ,J-1,bi,bj) & +vFld(I ,J ,bi,bj) * _dyC(I ,J ,bi,bj) & -vFld(I-1,J ,bi,bj) * _dyC(I-1,J ,bi,bj)) & * recip_rAz(I,J,bi,bj) & + & 0.25 _d 0 * (uFld(I,J,bi,bj)+uFld(I ,J-1,bi,bj)) & * ( _tanPhiAtU(I,J,bi,bj) + _tanPhiAtU(I,J-1,bi,bj) ) & *recip_rSphere & ) & *maskC(I ,J ,k,bi,bj)*maskC(I-1,J ,k,bi,bj) & *maskC(I ,J-1,k,bi,bj)*maskC(I-1,J-1,k,bi,bj) C one metric term is missing ENDDO ENDDO IF ( SEAICE_no_slip ) THEN C no slip boundary conditions apply only to e12Loc DO j=1-Oly+1,sNy+Oly DO i=1-Olx+1,sNx+Olx hFacU = _maskW(i,j,k,bi,bj) - _maskW(i,j-1,k,bi,bj) hFacV = _maskS(i,j,k,bi,bj) - _maskS(i-1,j,k,bi,bj) e12Loc(I,J,bi,bj) = e12Loc(I,J,bi,bj) & + recip_rAz(i,j,bi,bj) * 2. _d 0 * & ( hFacU * ( _dxC(i,j-1,bi,bj)*uFld(i,j ,bi,bj) & + _dxC(i,j, bi,bj)*uFld(i,j-1,bi,bj) ) & + hFacV * ( _dyC(i-1,j,bi,bj)*vFld(i ,j,bi,bj) & + _dyC(i, j,bi,bj)*vFld(i-1,j,bi,bj) ) ) & - hFacU & * 0.25 _d 0 * (uFld(I,J,bi,bj)+uFld(I ,J-1,bi,bj)) & * ( _tanPhiAtU(I,J,bi,bj) + _tanPhiAtU(I,J-1,bi,bj) ) & *recip_rSphere C one metric term is missing ENDDO ENDDO ENDIF ENDDO ENDDO #endif /* SEAICE_OLD_AND_BAD_DISCRETIZATION */ #endif /* SEAICE_ALLOW_DYNAMICS */ #endif /* SEAICE_CGRID */ RETURN END