--- trunk/tengDissertation/Introduction.tex	2006/06/21 16:43:07	2874
+++ trunk/tengDissertation/Introduction.tex	2006/06/23 20:21:54	2881
@@ -1114,23 +1114,10 @@ computer simulation. Figure
 (r)}{\rho}.
 \]
 Note that the delta function can be replaced by a histogram in
-computer simulation. Figure
-\ref{introFigure:pairDistributionFunction} shows a typical pair
-distribution function for the liquid argon system. The occurrence of
-several peaks in the plot of $g(r)$ suggests that it is more likely
-to find particles at certain radial values than at others. This is a
-result of the attractive interaction at such distances. Because of
-the strong repulsive forces at short distance, the probability of
-locating particles at distances less than about 3.7{\AA} from each
-other is essentially zero.
+computer simulation. Peaks in $g(r)$ represent solvent shells, and
+the height of these peaks gradually decreases to 1 as the liquid of
+large distance approaches the bulk density.
 
-%\begin{figure}
-%\centering
-%\includegraphics[width=\linewidth]{pdf.eps}
-%\caption[Pair distribution function for the liquid argon
-%]{Pair distribution function for the liquid argon}
-%\label{introFigure:pairDistributionFunction}
-%\end{figure}
 
 \subsubsection{\label{introSection:timeDependentProperties}\textbf{Time-dependent
 Properties}}