--- manual/s_algorithm/text/tracer.tex	2001/11/13 20:13:54	1.12
+++ manual/s_algorithm/text/tracer.tex	2004/03/23 16:47:04	1.15
@@ -1,4 +1,4 @@
-% $Header: /home/ubuntu/mnt/e9_copy/manual/s_algorithm/text/tracer.tex,v 1.12 2001/11/13 20:13:54 adcroft Exp $
+% $Header: /home/ubuntu/mnt/e9_copy/manual/s_algorithm/text/tracer.tex,v 1.15 2004/03/23 16:47:04 afe Exp $
 % $Name:  $
 
 \section{Tracer equations}
@@ -124,6 +124,9 @@
 
 \section{Linear advection schemes}
 \label{sect:tracer-advection}
+\begin{rawhtml}
+<!-- CMIREDIR:linear_advection_schemes: -->
+\end{rawhtml}
 
 \begin{figure}
 \resizebox{5.5in}{!}{\includegraphics{part2/advect-1d-lo.eps}}
@@ -450,7 +453,7 @@
 
 The DST3 method described above must be used in a forward-in-time
 manner and is stable for $0 \le |c| \le 1$. Although the scheme
-appears to be forward-in-time, it is in fact second order in time and
+appears to be forward-in-time, it is in fact third order in time and
 the accuracy increases with the Courant number! For low Courant
 number, DST3 produces very similar results (indistinguishable in
 Fig.~\ref{fig:advect-1d-lo}) to the linear third order method but for