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Mesoscopic models of lipid bilayers and bilayers with embedded ...

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12 Simulation method for coarse-grained <strong>lipid</strong>s<br />

a timestep at least three orders <strong>of</strong> magnitude larger than in atomistic molecular dynamics<br />

simulations, where a timestep <strong>of</strong> the order <strong>of</strong> few fs is typically used.<br />

In the next section we describe the coarse-grained model we use to represent <strong>lipid</strong><br />

molecules <strong>and</strong> we show that these model <strong>lipid</strong>s, simulated <strong>with</strong> DPD, spontaneously<br />

self-assemble into micelles <strong>and</strong> <strong>bilayers</strong>.<br />

2.2 Coarse-grained model <strong>of</strong> <strong>lipid</strong>s<br />

Within the mesoscopic approach, each molecule <strong>of</strong> the system (or groups <strong>of</strong> molecules)<br />

is coarse-grained by a set <strong>of</strong> beads. We consider three types <strong>of</strong> beads: a water-like<br />

bead (denoted as ’w’), which <strong>models</strong> the solvent, an hydrophilic bead (denoted as ’h’)<br />

which <strong>models</strong> a section <strong>of</strong> the <strong>lipid</strong> headgroup, <strong>and</strong> an hydrophobic bead (denoted<br />

as ’t’) which <strong>models</strong> a segment <strong>of</strong> the <strong>lipid</strong> hydrocarbon tail. A <strong>lipid</strong> is constructed<br />

by connecting head- <strong>and</strong> tail-beads <strong>with</strong> springs. The simplest <strong>lipid</strong> consists <strong>of</strong> a linear<br />

chain <strong>of</strong> one hydrophilic head-bead <strong>and</strong> one tail <strong>of</strong> hydrophobic beads. A more<br />

realistic model <strong>of</strong> a phospho<strong>lipid</strong> can be constructed by connecting two hydrophobic<br />

tails to an headgroup consisting <strong>of</strong> one or more head-beads. In both single- <strong>and</strong><br />

double-tail <strong>lipid</strong>s the tail(s) can have different length. We denote a single-tail <strong>lipid</strong><br />

<strong>with</strong> one head-bead <strong>and</strong> n tail beads as htn, <strong>and</strong> a double-tail <strong>lipid</strong> <strong>with</strong> m headbeads<br />

<strong>and</strong> n tail-beads as hm(tn)2 (see figure 2.1).<br />

Figure 2.1: Schematic drawing <strong>of</strong> the single- <strong>and</strong> double-tail model <strong>lipid</strong>s described in the text<br />

<strong>and</strong> their nomenclature. The black particles represent the hydrophilic head-beads <strong>and</strong> the<br />

white particles the hydrophobic tail-beads.<br />

A mapping <strong>of</strong> coarse-grained <strong>lipid</strong>s onto real phospho<strong>lipid</strong>s can be established<br />

through the factor Nm. We have chosen a mapping factor <strong>of</strong> Nm = 3, corresponding<br />

to three water molecules represented by one DPD-bead <strong>of</strong> volume <strong>of</strong> 90 ˚A 3 . In terms

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