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Revision 3943 by kstocke1, Mon Sep 2 20:34:55 2013 UTC vs.
Revision 3944 by kstocke1, Tue Sep 3 19:30:21 2013 UTC

# Line 2 | Line 2
2   \setkeys{acs}{usetitle = true}
3  
4   \usepackage{caption}
5 < \usepackage{float}
5 > \usepackage{endfloat}
6   \usepackage{geometry}
7   \usepackage{natbib}
8   \usepackage{setspace}
# Line 114 | Line 114 | of rectangular slabs. A temperature profile along the
114   The adaptation of VSS-RNEMD for non-periodic systems is relatively
115   straightforward. The major modifications to the method are the addition of a rotational shearing term and the use of more versatile hot / cold regions instead
116   of rectangular slabs. A temperature profile along the $r$ coordinate is created by recording the average temperature of concentric spherical shells.
117 +
118 + \begin{figure}
119 +        \center{\includegraphics[width=7in]{figures/VSS}}
120 +        \caption{Schematics of periodic (left) and nonperiodic (right) Velocity Shearing and Scaling RNEMD. A kinetic energy or momentum flux is applied from region B to region A. Thermal gradients are depicted by a color gradient. Linear or angular velocity gradients are shown as arrows.}
121 +        \label{fig:VSS}
122 + \end{figure}
123  
124   At each time interval, the particle velocities ($\mathbf{v}_i$ and
125   $\mathbf{v}_j$) in the cold and hot shells ($C$ and $H$) are modified by a

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