--- manual/s_algorithm/text/spatial-discrete.tex	2006/04/05 01:16:27	1.19
+++ manual/s_algorithm/text/spatial-discrete.tex	2006/06/28 16:55:53	1.21
@@ -1,4 +1,4 @@
-% $Header: /home/ubuntu/mnt/e9_copy/manual/s_algorithm/text/spatial-discrete.tex,v 1.19 2006/04/05 01:16:27 jmc Exp $
+% $Header: /home/ubuntu/mnt/e9_copy/manual/s_algorithm/text/spatial-discrete.tex,v 1.21 2006/06/28 16:55:53 jmc Exp $
 % $Name:  $
 
 \section{Spatial discretization of the dynamical equations}
@@ -13,8 +13,6 @@
 representation of the position of the boundary. We treat the
 horizontal and vertical directions as separable and differently.
 
-\input{part2/notation}
-
 
 \subsection{The finite volume method: finite volumes versus finite difference}
 \begin{rawhtml}
@@ -141,8 +139,8 @@
 grid for all panels. a) The area of a tracer cell, $A_c$, is bordered
 by the lengths $\Delta x_g$ and $\Delta y_g$. b) The area of a
 vorticity cell, $A_\zeta$, is bordered by the lengths $\Delta x_c$ and
-$\Delta y_c$. c) The area of a u cell, $A_c$, is bordered by the
-lengths $\Delta x_v$ and $\Delta y_f$. d) The area of a v cell, $A_c$,
+$\Delta y_c$. c) The area of a u cell, $A_w$, is bordered by the
+lengths $\Delta x_v$ and $\Delta y_f$. d) The area of a v cell, $A_s$,
 is bordered by the lengths $\Delta x_f$ and $\Delta y_u$.}
 \label{fig:hgrid}
 \end{figure}