128 |
|
kcal/mol}$. $V_{\text{dp}}$ is the dipole potential with |
129 |
|
$|\mu_{\text{w}}| = 2.35\text{ D}$. |
130 |
|
|
131 |
< |
The hydrogen bonding of the model is governed by the $V_{\text{sp}}$ term of the potentail. Its form is as follows: |
131 |
> |
The hydrogen bonding of the model is governed by the $V_{\text{sp}}$ |
132 |
> |
term of the potentail. Its form is as follows: |
133 |
|
\begin{equation} |
134 |
|
V_{\text{sp}}(\mathbf{r}_{i\!j},\boldsymbol{\Omega}_{i}, |
135 |
|
\boldsymbol{\Omega}_{j}) = |
166 |
|
$w^{x}_{ij}(\mathbf{r}_{ij},\boldsymbol{\Omega}_{i},\boldsymbol{\Omega}_{j})$ |
167 |
|
is needed because |
168 |
|
$w_{ij}(\mathbf{r}_{ij},\boldsymbol{\Omega}_{i},\boldsymbol{\Omega}_{j})$ |
169 |
< |
vanishes when $\theta_{ij}$ is $0^\circ$ or $180^\circ$. The angles $\theta_{ij}$ and $\phi_{ij}$ are defined by the spherical polar coordinates of the position of sphere $j$ in the reference frame fixed on sphere $i$ with the z-axis alligned with the dipole moment. |
169 |
> |
vanishes when $\theta_{ij}$ is $0^\circ$ or $180^\circ$. The angles |
170 |
> |
$\theta_{ij}$ and $\phi_{ij}$ are defined by the spherical polar |
171 |
> |
coordinates of the position of sphere $j$ in the reference frame fixed |
172 |
> |
on sphere $i$ with the z-axis alligned with the dipole moment. |
173 |
|
|
174 |
< |
Finaly, the sticky potentail is scaled by a cutoff function, $s(r_{ij})$ that scales smoothly between 0 and 1. It is represented by: |
174 |
> |
Finaly, the sticky potentail is scaled by a cutoff function, |
175 |
> |
$s(r_{ij})$ that scales smoothly between 0 and 1. It is represented |
176 |
> |
by: |
177 |
|
\begin{equation} |
178 |
|
s(r_{ij}) = |
179 |
|
\begin{cases} |
190 |
|
\subsection{The Phospholipid Model} |
191 |
|
\label{sec:lipidModel} |
192 |
|
|
193 |
+ |
\begin{floatingfigure}{90mm} |
194 |
+ |
\includegraphics[angle=-90,width=80mm]{lipidModel.epsi} |
195 |
+ |
\caption{A representation of the lipid model. $\phi$ is the torsion angle, $\theta$ is the bend angle, $\mu$ is the dipole moment of the head group, and n is the chain length. \vspace{5mm}} |
196 |
+ |
\label{fig:lipidModel} |
197 |
+ |
\end{floatingfigure} |
198 |
|
|
199 |
+ |
The lipid molecules in our simulations are unified atom models. Figure |
200 |
+ |
\ref{fig:lipidModel} shows a template drawing for one of our |
201 |
+ |
lipids. The Head group of the phospholipid is replaced by a single |
202 |
+ |
Lennard-Jones sphere with a freely oriented dipole placed at it's |
203 |
+ |
center. The magnitude of it's dipole moment is 20.6 D. The tail atoms |
204 |
+ |
are unifed $\text{CH}_2$ and $\text{CH}_3$ atoms and are also modeled |
205 |
+ |
as Lennard-Jones spheres. The total potential for the lipid is |
206 |
+ |
represented by Equation \ref{eq:lipidModelPot}. |
207 |
+ |
|
208 |
+ |
\begin{equation} |
209 |
+ |
V_{\mbox{lipid}} = \overbrace{% |
210 |
+ |
V_{\text{bend}}(\theta_{ijk}) +% |
211 |
+ |
V_{\text{tors.}}(\phi_{ijkl})}^{bonded} |
212 |
+ |
+ \overbrace{% |
213 |
+ |
V_{\text{LJ}}(r_{i\!j}) + |
214 |
+ |
V_{\text{dp}}(r_{i\!j},\Omega_{i},\Omega_{j})% |
215 |
+ |
}^{non-bonded} |
216 |
+ |
\label{eq:lipidModelPot} |
217 |
+ |
\end{equation} |
218 |
+ |
|
219 |
+ |
The non bonded interactions, $V_{\text{LJ}}$ and $V_{\text{dp}}$, are |
220 |
+ |
the Lennard-Jones and dipole-dipole interactions respectively. For the |
221 |
+ |
non-bonded potentials, only the bend and the torsional potentials are |
222 |
+ |
calculated. The bond potential is not calculated, and the bond lengths |
223 |
+ |
are constrained via RATTLE.\cite{leach01:mm} The bend potential is of |
224 |
+ |
the form: |
225 |
+ |
\begin{equation} |
226 |
+ |
V_{\text{bend}}(\theta_{ijk}) = k_{\theta}\frac{(\theta_{ijk} - \theta_0)^2}{2} |
227 |
+ |
\label{eq:bendPot} |
228 |
+ |
\end{equation} |
229 |
+ |
Where $k_{\theta}$ sets the stiffness of the bend potential, and $\theta_0$ |
230 |
+ |
sets the equilibrium bend angle. The torsion potential was given by: |
231 |
+ |
\begin{equation} |
232 |
+ |
V_{\text{tors.}}(\phi_{ijkl})= \cos(\phi_{ijkl}) |
233 |
+ |
\label{eq:torsPot} |
234 |
+ |
\end{equation} |
235 |
+ |
Here, ``blank'' controls the scaling of the torsion potential, and the |
236 |
+ |
$c$ terms are paramterized for the $\cos$ expansion. All parameters |
237 |
+ |
for bonded and non-bonded potentials in the tail atoms were taken from |
238 |
+ |
TraPPE.\cite{Siepmann1998} The bonded interactions for the head atom |
239 |
+ |
were also taken from TraPPE, however it's dipole moment and mass were |
240 |
+ |
based on the properties of ``DMPC?'''s head group. The Lennard-Jones |
241 |
+ |
parameter for the Head group was chosen such that it was roughly twice |
242 |
+ |
the size of a $\text{CH}_3$ atom, and it's well depth was set to be |
243 |
+ |
aproximately equal to that of $\text{CH}_3$. |
244 |
+ |
|
245 |
+ |
\section{Simulations} |
246 |
+ |
\subsection{25 lipids in water} |
247 |
+ |
|
248 |
+ |
\subsection{50 randomly oriented lipids in water} |
249 |
+ |
|
250 |
+ |
\section{Preliminary Results} |
251 |
+ |
|
252 |
+ |
\section{Discussion} |
253 |
+ |
|
254 |
+ |
\section{Future Directions} |
255 |
+ |
|
256 |
+ |
|
257 |
+ |
\pagebreak |
258 |
|
\bibliographystyle{achemso} |
259 |
< |
\bibliography{canidacy_paper} |
190 |
< |
\end{document} |
259 |
> |
\bibliography{canidacy_paper} \end{document} |