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root/group/trunk/oopsePaper/DUFF.tex
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4 \section{The DUFF Energy Functionals}
5 \label{sec:energyFunctionals}
6
7 The main energy functional set in OOPSE is DUFF (the Dipolar
8 Unified-atom Force Field). DUFF is a collection of parameters taken
9 from Seipmann \emph{et al.}\cite{Siepmann1998} and Ichiye \emph{et
10 al.}\cite{liu96:new_model} The total energy of interaction is given by
11 Eq.~\ref{eq:totalPotential}:
12 \begin{equation}
13 V_{\text{Total}} =
14 \overbrace{V_{\theta} + V_{\phi}}^{\text{bonded}} +
15 \underbrace{V_{\text{LJ}} + V_{\text{Dp}} + %
16 V_{\text{SSD}}}_{\text{non-bonded}} \label{eq:totalPotential}
17 \end{equation}
18
19 \subsection{Bonded Interactions}
20 \label{subSec:bondedInteractions}
21
22 The bonded interactions in the DUFF functional set are limited to the
23 bend potential and the torsional potential. Bond potentials are not
24 calculated, instead all bond lengths are fixed to allow for large time
25 steps to be taken between force evaluations.
26
27 The bend functional is of the form:
28 \begin{equation}
29 V_{\theta} = \sum k_{\theta}( \theta - \theta_0 )^2 \label{eq:bendPot}
30 \end{equation}
31 $k_{\theta}$, the force constant, and $\theta_0$, the equilibrium bend
32 angle, were taken from the TraPPE forcefield of Siepmann.
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34 The torsion functional has the form:
35 \begin{equation}
36 V_{\phi} = \sum ( k_1 \cos^3 \phi + k_2 \cos^2 \phi + k_3 \cos \phi + k_4)
37 \label{eq:torsionPot}
38 \end{equation}
39 Here, the authors decided to use a potential in terms of a power
40 expansion in $\cos \phi$ rather than the typical expansion in
41 $\phi$. This prevents the need for repeated trigonemtric
42 evaluations. Again, all $k_n$ constants were based on those in TraPPE.
43
44 \subsection{Non-Bonded Interactions}
45 \label{subSec:nonBondedInteractions}
46
47 \begin{equation}
48 V_{\text{LJ}} = \text{internal + external}
49 \end{equation}
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