148 |
\Delta z_{20}=815\,{\rm m} |
\Delta z_{20}=815\,{\rm m} |
149 |
$ (here the numeric subscript indicates the model level index number, ${\tt k}$). |
$ (here the numeric subscript indicates the model level index number, ${\tt k}$). |
150 |
The implicit free surface form of the pressure equation described in Marshall et. al |
The implicit free surface form of the pressure equation described in Marshall et. al |
151 |
\cite{Marshall97a} is employed. A Laplacian operator, $\nabla^2$, provides viscous |
\cite{marshall:97a} is employed. A Laplacian operator, $\nabla^2$, provides viscous |
152 |
dissipation. Thermal and haline diffusion is also represented by a Laplacian operator. |
dissipation. Thermal and haline diffusion is also represented by a Laplacian operator. |
153 |
|
|
154 |
Wind-stress forcing is added to the momentum equations for both |
Wind-stress forcing is added to the momentum equations for both |