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1  
2 + \section{The DUFF Energy Function}
3 + \label{sec:energyFunctionals}
4  
3 \section{The DUFF Energy Functionals}
5  
6 < The main energy functional set in OOPSE is DUFF (the Dipolar
6 >
7 > The main energy function in OOPSE is DUFF (the Dipolar
8   Unified-atom Force Field). DUFF is a collection of parameters taken
9 < from Seipman \emph{et al.}\cite{Siepmann1998}~and Ichiye \emph{et
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}.
11 > Eq.~\ref{eq:totalPotential}:
12   \begin{equation}
13 < V_{\text{lipid}} =
14 <        \sum_{i}V_{i}^{\text{internal}}
15 <        + \sum_i \sum_{j>i} \sum_{\alpha_i}
16 <        \sum_{\beta_j}
15 <        V_{\text{LJ}}(r_{\alpha_{i}\beta_{j}})
16 <        +\sum_i\sum_{j>i}V_{\text{dp}}(r_{1_i,1_j},\Omega_{1_i},\Omega_{1_j})
17 < \label{eq:totalPotential}
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.
33 +
34 + The torsion functional has the form:
35 + \begin{equation}
36 + V_{\phi} =  \sum ( k_3 \cos^3 \phi + k_2 \cos^2 \phi + k_1 \cos \phi + k_0)
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}
50 +
51 +

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