--- manual/s_algorithm/text/spatial-discrete.tex	2001/11/13 18:15:26	1.11
+++ manual/s_algorithm/text/spatial-discrete.tex	2004/03/23 16:47:04	1.14
@@ -1,4 +1,4 @@
-% $Header: /home/ubuntu/mnt/e9_copy/manual/s_algorithm/text/spatial-discrete.tex,v 1.11 2001/11/13 18:15:26 adcroft Exp $
+% $Header: /home/ubuntu/mnt/e9_copy/manual/s_algorithm/text/spatial-discrete.tex,v 1.14 2004/03/23 16:47:04 afe Exp $
 % $Name:  $
 
 \section{Spatial discretization of the dynamical equations}
@@ -14,6 +14,11 @@
 
 
 \subsection{The finite volume method: finite volumes versus finite difference}
+\begin{rawhtml}
+<!-- CMIREDIR:finite_volume: -->
+\end{rawhtml}
+
+
 
 The finite volume method is used to discretize the equations in
 space. The expression ``finite volume'' actually has two meanings; one
@@ -471,7 +476,7 @@
 \end{eqnarray}
 where the continuity equation has been most naturally discretized by
 staggering the three components of velocity as shown in
-Fig.~\ref{fig-cgrid3d}. The grid lengths $\Delta x_c$ and $\Delta y_c$
+Fig.~\ref{fig:cgrid3d}. The grid lengths $\Delta x_c$ and $\Delta y_c$
 are the lengths between tracer points (cell centers). The grid lengths
 $\Delta x_g$, $\Delta y_g$ are the grid lengths between cell
 corners. $\Delta r_f$ and $\Delta r_c$ are the distance (in units of