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

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98 <strong>Mesoscopic</strong> model for <strong>lipid</strong> <strong>bilayers</strong> <strong>with</strong> <strong>embedded</strong> proteins<br />

they do not take into full account the three dimensional structure <strong>of</strong> the bilayer), <strong>and</strong>,<br />

for example, they can not be used to investigate the <strong>lipid</strong>-induced protein tilting.<br />

Simulations on more realistic <strong>models</strong>, such as all-atom <strong>models</strong> for <strong>lipid</strong> <strong>bilayers</strong> <strong>with</strong><br />

<strong>embedded</strong> proteins, have anyway confirmed that, at least <strong>with</strong>in a time <strong>of</strong> the order<br />

<strong>of</strong> the nanoseconds, a mismatched protein may induce a deformation <strong>of</strong> the <strong>lipid</strong> bilayer<br />

structure [10, 63, 170], <strong>and</strong> that the deformation is <strong>of</strong> the exponential type [11].<br />

The same type <strong>of</strong> studies have also shown that—although to reduce a possible hydrophobic<br />

mismatch synthetic peptides may prefer to deform the <strong>lipid</strong> bilayer, rather<br />

than undergo tilting [171]—tilting may also occur for membrane peptides [7,8]. Incidentally,<br />

the results from these studies indicated that the helical-peptides experience<br />

a slight bend in the middle <strong>of</strong> the helix.<br />

No matter the huge body <strong>of</strong> experimental <strong>and</strong> theoretical studies on <strong>lipid</strong> <strong>bilayers</strong><br />

<strong>with</strong> <strong>embedded</strong> proteins, issues such as the range <strong>of</strong> the protein-induced <strong>lipid</strong> bilayer<br />

perturbation, its dependence on protein size, <strong>and</strong> the occurrence <strong>of</strong> protein tilting (or<br />

even bending) to adjust for hydrophobic mismatch, are still a matter <strong>of</strong> debate. Here<br />

we want to focus on these issues by adopting the DPD simulation method to study<br />

the behavior <strong>of</strong> a mesoscopic model for <strong>lipid</strong> <strong>bilayers</strong> <strong>with</strong> <strong>embedded</strong> proteins. We<br />

have focused our attention on the perturbation caused by a membrane protein on<br />

the surrounding <strong>lipid</strong>s, its possible dependence on hydrophobic mismatch, protein<br />

size, <strong>and</strong> on temperature. We have investigated whether <strong>and</strong> to which extent—due to<br />

hydrophobic mismatch <strong>and</strong> via the cooperative nature <strong>of</strong> the system—a protein may<br />

prefer to tilt (<strong>with</strong> respect to the normal to the bilayer plane), rather than to induce a<br />

bilayer deformation <strong>with</strong>out (or even <strong>with</strong>) tilting.<br />

7.2 Computational details<br />

7.2.1 Lipid <strong>and</strong> protein <strong>models</strong><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. In particular, to model the bilayer <strong>and</strong> the<br />

<strong>embedded</strong> proteins, we consider three types <strong>of</strong> beads: a water-like bead, labeled ’w’;<br />

a hydrophilic bead, labeled ’h’, which <strong>models</strong> a part <strong>of</strong> the headgroup <strong>of</strong> either the<br />

<strong>lipid</strong> or the protein; <strong>and</strong> a hydrophobic bead, labeled either ’tL’ or ’tP’, depending on<br />

whether it refers to a portion <strong>of</strong> the <strong>lipid</strong> hydrocarbon chain or a portion <strong>of</strong> the hydrophobic<br />

region <strong>of</strong> protein, respectively. The systems that we have simulated are<br />

made <strong>of</strong> model <strong>lipid</strong>s having three headgroup beads <strong>and</strong> two tails <strong>of</strong> five beads each;<br />

this corresponds to the case <strong>of</strong> acyl chains <strong>with</strong> fourteen carbon atoms, namely to a<br />

model for a dimyristoylphosphatidylcholine (DMPC) phospho<strong>lipid</strong>, as illustrated in<br />

figure 2.2 <strong>of</strong> Chapter 2, <strong>and</strong> in figure 7.1(a). Within the model formulation, a protein<br />

is considered as a rod-like object, <strong>with</strong> no appreciable internal flexibility, <strong>and</strong> characterized<br />

by a hydrophobic length dP. The model for the transmembrane protein is

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