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