| 22 |
#include "PARAMS.h" |
#include "PARAMS.h" |
| 23 |
#include "GRID.h" |
#include "GRID.h" |
| 24 |
#include "SEAICE_PARAMS.h" |
#include "SEAICE_PARAMS.h" |
| 25 |
|
#include "SEAICE.h" |
| 26 |
|
|
| 27 |
#ifdef ALLOW_AUTODIFF_TAMC |
#ifdef ALLOW_AUTODIFF_TAMC |
| 28 |
# include "tamc.h" |
# include "tamc.h" |
| 55 |
INTEGER i, j, bi, bj |
INTEGER i, j, bi, bj |
| 56 |
C hFacU, hFacV - determine the no-slip boundary condition |
C hFacU, hFacV - determine the no-slip boundary condition |
| 57 |
INTEGER k |
INTEGER k |
| 58 |
_RS hFacU, hFacV |
_RS hFacU, hFacV, noSlipFac |
| 59 |
|
|
| 60 |
k = 1 |
k = 1 |
| 61 |
|
noSlipFac = 0. _d 0 |
| 62 |
|
IF ( SEAICE_no_slip ) noSlipFac = 1. _d 0 |
| 63 |
C |
C |
| 64 |
|
#ifndef SEAICE_OLD_AND_BAD_DISCRETIZATION |
| 65 |
|
DO bj=myByLo(myThid),myByHi(myThid) |
| 66 |
|
DO bi=myBxLo(myThid),myBxHi(myThid) |
| 67 |
|
DO j=1-Oly,sNy+Oly-1 |
| 68 |
|
DO i=1-Olx,sNx+Olx-1 |
| 69 |
|
C evaluate strain rates |
| 70 |
|
e11(I,J,bi,bj) = _recip_dxF(I,J,bi,bj) * |
| 71 |
|
& (uFld(I+1,J,1,bi,bj)-uFld(I,J,1,bi,bj)) |
| 72 |
|
& +HALF* |
| 73 |
|
& (vFld(I,J,1,bi,bj)+vFld(I,J+1,1,bi,bj)) |
| 74 |
|
& * k2AtC(I,J,bi,bj) |
| 75 |
|
e22(I,J,bi,bj) = _recip_dyF(I,J,bi,bj) * |
| 76 |
|
& (vFld(I,J+1,1,bi,bj)-vFld(I,J,1,bi,bj)) |
| 77 |
|
& +HALF* |
| 78 |
|
& (uFld(I,J,1,bi,bj)+uFld(I+1,J,1,bi,bj)) |
| 79 |
|
& * k1AtC(I,J,bi,bj) |
| 80 |
|
C one metric term is missing |
| 81 |
|
ENDDO |
| 82 |
|
ENDDO |
| 83 |
|
DO j=1-Oly+1,sNy+Oly |
| 84 |
|
DO i=1-Olx+1,sNx+Olx |
| 85 |
|
hFacU = _maskW(i,j,k,bi,bj) - _maskW(i,j-1,k,bi,bj) |
| 86 |
|
hFacV = _maskS(i,j,k,bi,bj) - _maskS(i-1,j,k,bi,bj) |
| 87 |
|
e12(I,J,bi,bj) = HALF*( |
| 88 |
|
& ( uFld(I,J,1,bi,bj) - uFld(I ,J-1,1,bi,bj) ) |
| 89 |
|
& * _recip_dyU(I,J,bi,bj) |
| 90 |
|
& + ( vFld(I,J,1,bi,bj) - vFld(I-1,J ,1,bi,bj) ) |
| 91 |
|
& * _recip_dxV(I,J,bi,bj) |
| 92 |
|
& - k1AtZ(I,J,bi,bj) |
| 93 |
|
& * 0.5 _d 0 * (vFld(I,J,1,bi,bj)+vFld(I-1,J ,1,bi,bj)) |
| 94 |
|
& - k2AtZ(I,J,bi,bj) |
| 95 |
|
& * 0.5 _d 0 * (uFld(I,J,1,bi,bj)+uFld(I ,J-1,1,bi,bj)) |
| 96 |
|
& ) |
| 97 |
|
& *maskC(I ,J ,k,bi,bj)*maskC(I-1,J ,k,bi,bj) |
| 98 |
|
& *maskC(I ,J-1,k,bi,bj)*maskC(I-1,J-1,k,bi,bj) |
| 99 |
|
& + 2.0 _d 0 * noSlipFac * ( |
| 100 |
|
& ( uFld(I,J,1,bi,bj) + uFld(I ,J-1,1,bi,bj) ) |
| 101 |
|
& * _recip_dyU(I,J,bi,bj) * hFacU |
| 102 |
|
& + ( vFld(I,J,1,bi,bj) + vFld(I-1,J ,1,bi,bj) ) |
| 103 |
|
& * _recip_dxV(I,J,bi,bj) * hFacV |
| 104 |
|
& ) |
| 105 |
|
C no slip at the boundary implies u(j)+u(j-1)=0 and v(i)+v(i-1)=0 |
| 106 |
|
C accross the boundary; this is already accomplished by masking so |
| 107 |
|
C that the following lines are not necessary |
| 108 |
|
c$$$ & - hFacV * k1AtZ(I,J,bi,bj) |
| 109 |
|
c$$$ & * 0.5 _d 0 * (vFld(I,J,1,bi,bj)+vFld(I-1,J ,1,bi,bj)) |
| 110 |
|
c$$$ & - hFacU * k2AtZ(I,J,bi,bj) |
| 111 |
|
c$$$ & * 0.5 _d 0 * (uFld(I,J,1,bi,bj)+uFld(I ,J-1,1,bi,bj)) |
| 112 |
|
ENDDO |
| 113 |
|
ENDDO |
| 114 |
|
|
| 115 |
|
c$$$ ENDIF |
| 116 |
|
ENDDO |
| 117 |
|
ENDDO |
| 118 |
|
#else |
| 119 |
|
C this the old and incomplete discretization, here I also erroneously |
| 120 |
|
C used finite-volumes to discretize the strain rates |
| 121 |
DO bj=myByLo(myThid),myByHi(myThid) |
DO bj=myByLo(myThid),myByHi(myThid) |
| 122 |
DO bi=myBxLo(myThid),myBxHi(myThid) |
DO bi=myBxLo(myThid),myBxHi(myThid) |
| 123 |
DO j=1-Oly,sNy+Oly-1 |
DO j=1-Oly,sNy+Oly-1 |
| 175 |
ENDIF |
ENDIF |
| 176 |
ENDDO |
ENDDO |
| 177 |
ENDDO |
ENDDO |
| 178 |
|
#endif /* SEAICE_OLD_AND_BAD_DISCRETIZATION */ |
| 179 |
#endif /* SEAICE_ALLOW_DYNAMICS */ |
#endif /* SEAICE_ALLOW_DYNAMICS */ |
| 180 |
#endif /* SEAICE_CGRID */ |
#endif /* SEAICE_CGRID */ |
| 181 |
RETURN |
RETURN |