43 |
everywhere else. This term is therefore referred to as the surface |
everywhere else. This term is therefore referred to as the surface |
44 |
correction term. Global conservation is not possible using the |
correction term. Global conservation is not possible using the |
45 |
flux-form (as here) and a linearized free-surface |
flux-form (as here) and a linearized free-surface |
46 |
(\cite{Griffies00,Campin02}). |
(\cite{griffies:00,campin:02}). |
47 |
|
|
48 |
The continuity equation can be recovered by setting |
The continuity equation can be recovered by setting |
49 |
$G_{diff}=G_{forc}=0$ and $\tau=1$. |
$G_{diff}=G_{forc}=0$ and $\tau=1$. |
200 |
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|
201 |
For non-divergent flow, this discretization can be shown to conserve |
For non-divergent flow, this discretization can be shown to conserve |
202 |
the tracer both locally and globally and to globally conserve tracer |
the tracer both locally and globally and to globally conserve tracer |
203 |
variance, $\tau^2$. The proof is given in \cite{Adcroft95,Adcroft97}. |
variance, $\tau^2$. The proof is given in \cite{adcroft:95,adcroft:97}. |
204 |
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205 |
\fbox{ \begin{minipage}{4.75in} |
\fbox{ \begin{minipage}{4.75in} |
206 |
{\em S/R GAD\_C2\_ADV\_X} ({\em gad\_c2\_adv\_x.F}) |
{\em S/R GAD\_C2\_ADV\_X} ({\em gad\_c2\_adv\_x.F}) |