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Revision 971 by mmeineke, Wed Jan 21 02:25:18 2004 UTC vs.
Revision 1001 by mmeineke, Sat Jan 31 22:10:21 2004 UTC

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5   \section{\label{lipidSec:Intro}Introduction}
6  
7 + In the past 10 years, computer speeds have allowed for the atomistic
8 + simulation of phospholipid bilayers.  These simulations have ranged
9 + from simulation of the gel phase ($L_{\beta}$) of
10 + dipalmitoylphosphatidylcholine (DPPC), \cite{Lindahl:2000} to the
11 + spontaneous aggregation of DPPC molecules into fluid phase
12 + ($L_{\alpha}$ bilayers. \cite{Marrinck:2001} With the exception of a
13 + few ambitious
14 + simulations,\cite{Marrinch:2001b,Marrinck:2002,Lindahl:2000} most
15 + investigations are limited to 64 to 256
16 + phospholipids.\cite{Lindal:2000,Sum:2003,Venable:2000,Gomez:2003,Smondyrev:1999,Marrinck:2001a}
17 + This is due to the expense of the computer calculations involved when
18 + performing these simulations.  To properly hydrate a bilayer, one
19 + typically needs 25 water molecules for every lipid, bringing the total
20 + number of atoms simulated to roughly 8,000 for a system of 64 DPPC
21 + molecules. Added to the difficluty is the electrostatic nature of the
22 + phospholipid head groups and water, requiring the computationally
23 + expensive Ewald sum or its slightly faster derivative particle mesh
24 + Ewald sum.\cite{Nina:2002,Norberg:2000,Patra:2003} These factors all
25 + limit the potential size and time lenghts of bilayer simulations.
26 +
27 + Unfortunately, much of biological interest happens on time and length
28 + scales unfeasible with current simulation. One such example is the
29 + observance of a ripple phase ($P_{\beta'}$) between the $L_{\beta}$
30 + and $L_{\alpha}$ phases of certain phospholipid
31 + bilayers.\cite{Katsaras:2000,Sengupta:2000} These ripples are shown to
32 + have periodicity on the order of 100-200~$\mbox{\AA}$. A simulation on
33 + this length scale would have approximately 1,300 lipid molecules with
34 + an additional 25 water molecules per lipid to fully solvate the
35 + bilayer. A simulation of this size is impractical with current
36 + atomistic models.
37 +
38 + Another class of simulations to consider, are those dealing with the
39 + diffusion of molecules through a bilayer.  Due to the fluid-like
40 + properties of a lipid membrane, not all diffusion across the membrane
41 + happens at pores.  Some molecules of interest may incorporate
42 + themselves directly into the membrane.  Once here, they may possess an
43 + appreciable waiting time (on the order of 10's to 100's of
44 + nanoseconds) within the bilayer.  Such long simulation times are
45 + difficulty to obtain when integrating the system with atomistic
46 + detail.
47 +
48 + Addressing these issues, several schemes have been proposed.  One
49 + approach by Goetz and Liposky\cite{Goetz:1998} is to model the entire
50 + system as Lennard-Jones spheres. Phospholipids are represented by
51 + chains of beads with the top most beads identified as the head
52 + atoms. Polar and non-polar interactions are mimicked through
53 + attractive and soft-repulsive potentials respectively.  A similar
54 + model proposed by Marrinck \emph{et. al.}\cite{Marrinck:2004}~ uses a
55 + similar technique for modeling polar and non-polar interactions with
56 + Lennard-Jones spheres. However, they also include charges on the head
57 + group spheres to mimic the electrostatic interactions of the
58 + bilayer. While the solvent spheres are kept charge-neutral and
59 + interact with the bilayer solely through an attractive Lennard-Jones
60 + potential.
61 +
62 + The model used in this investigation adds more information to the
63 + interactions than the previous two models,
64 +
65   \section{\label{lipidSec:Methods}Methods}
66  
67   \subsection{\label{lipidSec:lipidMedel}The Lipid Model}

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