| 80 |
\>\> CALC\_GRAD\_PHI\_SURF \` $\nabla \eta^{n+1}$ \\ |
\>\> CALC\_GRAD\_PHI\_SURF \` $\nabla \eta^{n+1}$ \\ |
| 81 |
\>\> CORRECTION\_STEP \` $u^{n+1}$,$v^{n+1}$ (\ref{eq:un+1-rigid-lid},\ref{eq:vn+1-rigid-lid}) |
\>\> CORRECTION\_STEP \` $u^{n+1}$,$v^{n+1}$ (\ref{eq:un+1-rigid-lid},\ref{eq:vn+1-rigid-lid}) |
| 82 |
\end{tabbing} \end{minipage} } \end{center} |
\end{tabbing} \end{minipage} } \end{center} |
| 83 |
\caption{Calling tree for the pressure method algorihtm} |
\caption{Calling tree for the pressure method algorihtm} |
| 84 |
\label{fig:call-tree-pressure-method} |
\label{fig:call-tree-pressure-method} |
| 85 |
\end{figure} |
\end{figure} |
| 86 |
|
|
| 554 |
{\em PARM01} of {\em data}. |
{\em PARM01} of {\em data}. |
| 555 |
|
|
| 556 |
The only difficulty with this approach is apparent in equation |
The only difficulty with this approach is apparent in equation |
| 557 |
$\ref{eq:Gt-n-staggered}$ and illustrated by the dotted arrow |
\ref{eq:Gt-n-staggered} and illustrated by the dotted arrow |
| 558 |
connecting $u,v^n$ with $G_\theta^{n-1/2}$. The flow used to advect |
connecting $u,v^n$ with $G_\theta^{n-1/2}$. The flow used to advect |
| 559 |
tracers around is not naturally located in time. This could be avoided |
tracers around is not naturally located in time. This could be avoided |
| 560 |
by applying the Adams-Bashforth extrapolation to the tracer field |
by applying the Adams-Bashforth extrapolation to the tracer field |
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