--- trunk/ssdePaper/nptSSD.tex	2004/02/07 00:16:47	1039
+++ trunk/ssdePaper/nptSSD.tex	2004/02/09 14:42:27	1040
@@ -46,7 +46,7 @@ experimental water very well in both the normal and su
 calculated densities which were were significantly lower than
 experimental densities.  Analysis of self-diffusion constants shows
 that the original SSD model captures the transport properties of
-experimental water very well in both the normal and super-cooled
+experimental water very well in both the normal and supercooled
 liquid regimes.  We also present our reparameterized versions of SSD
 for use both with the reaction field or without any long-range
 electrostatic corrections.  These are called the SSD/RF and SSD/E
@@ -739,7 +739,7 @@ Fig. \ref{ssdedense} shows the density profile for the
 \end{center}
 \end{figure} 
 
-Fig. \ref{ssdedense} shows the density profile for the SSD/E
+Figure \ref{ssdedense} shows the density profile for the SSD/E
 model in comparison to SSD1 without a reaction field, other
 common water models, and experimental results. The calculated
 densities for both SSD/E and SSD1 have increased
@@ -752,7 +752,7 @@ improved the structuring of the liquid (as seen in fig
 better than the SSD value of 0.967$\pm$0.003 g/cm$^3$. The
 changes to the dipole moment and sticky switching functions have
 improved the structuring of the liquid (as seen in figure
-\ref{grcompare}, but they have shifted the density maximum to much
+\ref{grcompare}), but they have shifted the density maximum to much
 lower temperatures. This comes about via an increase in the liquid
 disorder through the weakening of the sticky potential and
 strengthening of the dipolar character. However, this increasing
