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

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52 Structural characterization <strong>of</strong> <strong>lipid</strong> <strong>bilayers</strong><br />

where the tails are already very disordered, does not change the packing structure <strong>of</strong><br />

the bilayer <strong>and</strong> has no effect on the pressure pr<strong>of</strong>ile.<br />

As in the case <strong>of</strong> flexible <strong>lipid</strong>s, a modification in the tail end <strong>of</strong> stiff <strong>lipid</strong>s (figure<br />

4.9) does not change the pressure pr<strong>of</strong>ile, while a kink near the headgroup has a large<br />

effect. It is interesting to note that, while for flexible <strong>lipid</strong>s the main effect is in the<br />

interfacial region, for stiff <strong>lipid</strong>s the main effect is in the hydrophobic core. This difference<br />

can be easily explained. The considered <strong>bilayers</strong> formed by stiff, linear <strong>lipid</strong>s,<br />

are largely interdigitated, <strong>and</strong> interdigitated <strong>bilayers</strong> are more compact <strong>and</strong> ordered<br />

than <strong>bilayers</strong> formed by flexible <strong>lipid</strong>s. A kink near the <strong>lipid</strong>s headgroup destabilizes<br />

the interfacial region, decreasing the extent <strong>of</strong> interdigitation <strong>and</strong> increasing the disorder<br />

in the terminal region <strong>of</strong> the hydrophobic chains. This leads to a pressure pr<strong>of</strong>ile<br />

more similar to the one <strong>of</strong> fully flexible chains, <strong>with</strong> a minimum <strong>of</strong> the lateral<br />

pressure at the bilayer center. It is interesting to note that this effect is larger for the<br />

shorter chain.<br />

Our results are in general agreement <strong>with</strong> the mean field calculations <strong>of</strong> Cantor<br />

[94]. In [94] the effects <strong>of</strong> unsaturated bonds was studied by imposing a preference<br />

for a 90 o angle between three subsequent sites compared to 180 o used for a saturated<br />

chain. Also Cantor found that the largest changes in the lateral pressure distribution<br />

are obtained by modifications in the <strong>lipid</strong> topology close to the head group, <strong>and</strong> that<br />

the changes are more pronounced in short chains than in long ones.<br />

π(z)<br />

0.1<br />

0.0<br />

−0.1<br />

−0.2<br />

−7 −5 −3 −1 1 3 5 7<br />

Z<br />

(a)<br />

ht (L)<br />

4 t<br />

ht (L)<br />

3 t(K) t<br />

ht (K) t (L)<br />

3 t<br />

π(z)<br />

0.1<br />

0.0<br />

−0.1<br />

−0.2<br />

−7 −5 −3 −1 1 3 5 7<br />

Z<br />

(b)<br />

ht (L)<br />

8 t<br />

ht (L)<br />

7 t(K) t<br />

ht (K) t (L)<br />

7 t<br />

Figure 4.9: Pressure pr<strong>of</strong>ile, π(z), as function <strong>of</strong> the distance z from the bilayer center (z=0).<br />

Stiff <strong>lipid</strong>s <strong>and</strong> <strong>lipid</strong>s <strong>with</strong> a kink near the headgroup or at the tail end are compared for (a)<br />

short <strong>lipid</strong>s <strong>with</strong> 5 tail beads, <strong>and</strong> (b) long <strong>lipid</strong>s <strong>with</strong> 9 tail beads.

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