--- MITgcm/pkg/seaice/seaice_calc_strainrates.F 2009/03/18 10:26:49 1.10 +++ MITgcm/pkg/seaice/seaice_calc_strainrates.F 2009/03/18 12:58:17 1.11 @@ -1,4 +1,4 @@ -C $Header: /home/ubuntu/mnt/e9_copy/MITgcm/pkg/seaice/seaice_calc_strainrates.F,v 1.10 2009/03/18 10:26:49 mlosch Exp $ +C $Header: /home/ubuntu/mnt/e9_copy/MITgcm/pkg/seaice/seaice_calc_strainrates.F,v 1.11 2009/03/18 12:58:17 mlosch Exp $ C $Name: $ #include "SEAICE_OPTIONS.h" @@ -22,6 +22,7 @@ #include "PARAMS.h" #include "GRID.h" #include "SEAICE_PARAMS.h" +#include "SEAICE.h" #ifdef ALLOW_AUTODIFF_TAMC # include "tamc.h" @@ -54,10 +55,69 @@ INTEGER i, j, bi, bj C hFacU, hFacV - determine the no-slip boundary condition INTEGER k - _RS hFacU, hFacV + _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 + e11(I,J,bi,bj) = _recip_dxF(I,J,bi,bj) * + & (uFld(I+1,J,1,bi,bj)-uFld(I,J,1,bi,bj)) + & +HALF* + & (vFld(I,J,1,bi,bj)+vFld(I,J+1,1,bi,bj)) + & * k2AtC(I,J,bi,bj) + e22(I,J,bi,bj) = _recip_dyF(I,J,bi,bj) * + & (vFld(I,J+1,1,bi,bj)-vFld(I,J,1,bi,bj)) + & +HALF* + & (uFld(I,J,1,bi,bj)+uFld(I+1,J,1,bi,bj)) + & * k1AtC(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 + 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) + e12(I,J,bi,bj) = HALF*( + & ( uFld(I,J,1,bi,bj) - uFld(I ,J-1,1,bi,bj) ) + & * _recip_dyU(I,J,bi,bj) + & + ( vFld(I,J,1,bi,bj) - vFld(I-1,J ,1,bi,bj) ) + & * _recip_dxV(I,J,bi,bj) + & - k1AtZ(I,J,bi,bj) + & * 0.5 _d 0 * (vFld(I,J,1,bi,bj)+vFld(I-1,J ,1,bi,bj)) + & - k2AtZ(I,J,bi,bj) + & * 0.5 _d 0 * (uFld(I,J,1,bi,bj)+uFld(I ,J-1,1,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,1,bi,bj) + uFld(I ,J-1,1,bi,bj) ) + & * _recip_dyU(I,J,bi,bj) * hFacU + & + ( vFld(I,J,1,bi,bj) + vFld(I-1,J ,1,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,1,bi,bj)+vFld(I-1,J ,1,bi,bj)) +c$$$ & - hFacU * k2AtZ(I,J,bi,bj) +c$$$ & * 0.5 _d 0 * (uFld(I,J,1,bi,bj)+uFld(I ,J-1,1,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 @@ -115,6 +175,7 @@ ENDIF ENDDO ENDDO +#endif /* SEAICE_OLD_AND_BAD_DISCRETIZATION */ #endif /* SEAICE_ALLOW_DYNAMICS */ #endif /* SEAICE_CGRID */ RETURN