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Revision 101 by mmeineke, Tue Aug 27 02:32:29 2002 UTC vs.
Revision 102 by mmeineke, Tue Aug 27 20:54:03 2002 UTC

# Line 229 | Line 229 | V_{\text{tors.}}(\phi_{ijkl})= \cos(\phi_{ijkl})
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})
232 > V_{\text{tors.}}(\phi_{ijkl})= c_1[1+\cos\phi]
233 >        + c_2 [1 - \cos(2\phi)] + c_3[1 + \cos(3\phi)]
234   \label{eq:torsPot}
235   \end{equation}
236 < Here, ``blank'' controls the scaling of the torsion potential, and the
237 < $c$ terms are paramterized for the $\cos$ expansion. All parameters
238 < for bonded and non-bonded potentials in the tail atoms were taken from
239 < TraPPE.\cite{Siepmann1998} The bonded interactions for the head atom
240 < were also taken from TraPPE, however it's dipole moment and mass were
241 < based on the properties of ``DMPC?'''s head group. The Lennard-Jones
242 < 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 $\text{CH}_3$.
236 > All parameters for bonded and non-bonded potentials in the tail atoms
237 > were taken from TraPPE.\cite{Siepmann1998} The bonded interactions for
238 > the head atom were also taken from TraPPE, however it's dipole moment
239 > and mass were based on the properties of ``DMPC?'''s head group. The
240 > Lennard-Jones parameter for the head group was chosen such that it was
241 > roughly twice the size of a $\text{CH}_3$ atom, and it's well depth
242 > was set to be aproximately equal to that of $\text{CH}_3$.
243  
244 < \section{Simulations}
245 < \subsection{25 lipids in water}
244 > \section{Initial Simulation: 25 lipids in water}
245 > \label{sec:5x5}
246  
247 < \subsection{50 randomly oriented lipids in water}
247 > \subsection{Starting Configurtion and Parameters}
248 > \label{sec:5x5Start}
249 >
250 > \begin{floatingfigure}{85mm}
251 > \includegraphics[width=75mm]{5x5-initial.eps}
252 > \caption{A snapshot of the initial configuration of the 25 lipid simulation.}
253 > \label{fig:5x5Start}
254 > \end{floatingfigure}
255 >
256 > Our first simulation was an array of 25 single chained lipids in a sea
257 > of water (Figure \ref{fig:5x5Start}). The total number of water
258 > molecules was 1386, giving a final of water concentration of 70\%
259 > wt. The simulation box measured 34.5~$\mbox{\AA}$ x 39.4~$\mbox{\AA}$
260 > x 39.4~$\mbox{\AA}$ with periodic boundry connditions invoked. The
261 > system was simulated in the micro-canonical (NVE) ensemble with an
262 > average temperature of 300~K.
263 >
264 >
265 > yada
266 >
267 > yada
268  
269 + yada
270 + yya
271 + d
272 +
273 + uada
274 +
275 + adsd
276 +
277 + asfa
278 +
279 + asfdads
280 +
281 + \subsection{Results}
282 + \label{sec:5x5Results}
283 +
284 +
285 + Figure \ref{fig:5x5Final} shows a snapshot of the system at
286 + 3.6~ns. Here the bylayer has formed with the lipid chains tilted to
287 + the bylayer normal.
288 +
289 + yada
290 +
291 + yada
292 +
293 + yada
294 +
295 + yada
296 +
297 + %\begin{floatingfigure}{85mm}
298 + %\includegraphics[angle=-90,width=75mm]{5x5-3.6ns.epsi}
299 + %\caption{A snapshot of the system at 3.6~ns.\vspace{5mm}}
300 + %\label{fig:5x5Final}
301 + %\end{floatingfigure}
302 +
303 +
304 +
305 +
306 + \section{Second Simulation: 50 randomly oriented lipids in water}
307 +
308 + the second simulation
309 +
310   \section{Preliminary Results}
311  
312   \section{Discussion}

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