--- trunk/langevinHull/langevinHull.tex	2010/11/17 20:59:25	3701
+++ trunk/langevinHull/langevinHull.tex	2010/11/17 21:06:04	3702
@@ -672,7 +672,7 @@ Higher applied pressures de-structure the outermost la
 of water adjacent to the surface and
 the density of gold at the surface as a function of pressure.
 
-Higher applied pressures de-structure the outermost layer of the gold nanoparticle and the water at the metal/water interface. Increased pressure shows more overlap of the gold and water densities, indicating a less well-defined interfacial surface.
+Higher applied pressures de-structure the outermost layer of the gold nanoparticle and the water at the metal/water interface. Simulations at increased pressures have greater overlap of the gold and water densities, indicating a less well-defined interfacial surface.
 
 \begin{figure}
 \includegraphics[width=\linewidth]{RhoR}
@@ -680,7 +680,7 @@ At higher pressures, problems with the gold - water in
 \label{fig:RhoR}
 \end{figure}
 
-At higher pressures, problems with the gold - water interaction
+Indeed, at even higher pressures, problems with the gold - water interaction
 potential became apparent.  The model we are using (due to Spohr) was
 intended for relatively low pressures; it utilizes both shifted Morse
 and repulsive Morse potentials to model the Au/O and Au/H
