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Revision 1479 by chrisfen, Mon Sep 20 20:57:46 2004 UTC vs.
Revision 1485 by chrisfen, Tue Sep 21 18:27:12 2004 UTC

# Line 105 | Line 105 | that are 0.07 g/cm$^3$ less dense on average than ice
105  
106   \begin{figure}
107   \includegraphics[width=\linewidth]{unitCell.eps}
108 < \caption{Unit cells for (A) Ice-{\it i} and (B) Ice-$i^\prime$, the
109 < elongated variant of Ice-{\it i}.  The spheres represent the
108 > \caption{Unit cells for (A) Ice-{\it i} and (B) Ice-{\it i}$^\prime$,
109 > the elongated variant of Ice-{\it i}.  The spheres represent the
110   center-of-mass locations of the water molecules.  The $a$ to $c$
111   ratios for Ice-{\it i} and Ice-{\it i}$^\prime$ are given by
112   $a:2.1214c$ and $a:1.7850c$ respectively.}
# Line 138 | Line 138 | be noted that a second version of Ice-{\it i} (Ice-$i^
138   from which Ice-{\it i} was crystallized (SSD/E) in addition to several
139   common water models (TIP3P, TIP4P, TIP5P, and SPC/E) and a reaction
140   field parametrized single point dipole water model (SSD/RF). It should
141 < be noted that a second version of Ice-{\it i} (Ice-$i^\prime$) was
142 < used in calculations involving SPC/E, TIP4P, and TIP5P. The unit cell
143 < of this crystal (Fig. \ref{iceiCell}B) is similar to the Ice-{\it i}
144 < unit it is extended in the direction of the (001) face and compressed
145 < along the other two faces.
141 > be noted that a second version of Ice-{\it i} (Ice-{\it i}$^\prime$)
142 > was used in calculations involving SPC/E, TIP4P, and TIP5P. The unit
143 > cell of this crystal (Fig. \ref{iceiCell}B) is similar to the Ice-{\it
144 > i} unit it is extended in the direction of the (001) face and
145 > compressed along the other two faces.  There is typically a small
146 > distortion of proton ordered Ice-{\it i}$^\prime$ that converts the
147 > normally square tetramer into a rhombus with alternating approximately
148 > 85 and 95 degree angles.  The degree of this distortion is model
149 > dependent and significant enough to split the tetramer diagonal
150 > location peak in the radial distibution function.
151  
152   \section{Methods}
153  

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