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

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6.3 Results <strong>and</strong> Discussion 85<br />

ρ(z)<br />

0.3<br />

0.2<br />

0.1<br />

0.0<br />

−0.1<br />

−6 −4 −2 0<br />

Z<br />

2 4 6<br />

0.0<br />

−0.1<br />

(a) Pure bilayer<br />

−0.2<br />

−6 −4 −2 0<br />

Z<br />

2 4 6<br />

w<br />

h<br />

t (1,..,n−1)<br />

t n<br />

ρ tot<br />

0.3 w<br />

h<br />

0.2<br />

t (1,..,n−1)<br />

tn db<br />

0.1<br />

π(z)<br />

(c) dbA<br />

0.3 w<br />

h<br />

0.2<br />

t (1,..,n−1)<br />

tn db<br />

0.1<br />

π(z)<br />

0.0<br />

−0.1<br />

−0.2<br />

−6 −4 −2 0<br />

Z<br />

2 4 6<br />

0.0<br />

−0.1<br />

(b) dbH<br />

0.3 w<br />

h<br />

0.2<br />

t (1,..,n−1)<br />

tn db<br />

0.1<br />

π(z)<br />

−0.2<br />

−6 −4 −2 0<br />

Z<br />

2 4 6<br />

(d) dbN<br />

Figure 6.3: Density pr<strong>of</strong>iles for the pure ht (L)<br />

6 t bilayer (a), <strong>and</strong> for the same bilayer <strong>with</strong> (b)<br />

hydrophobic (dbH), (c) amphiphilic (dbA), <strong>and</strong> (d) neutral dumb-bells (dbN). In figures (b),<br />

(c) <strong>and</strong> (d) the lateral pressure pr<strong>of</strong>ile π(z) <strong>of</strong> the pure bilayer is also plotted. Note that the<br />

densities have been rescaled to fit in the same scale as the lateral pressure (hence the values<br />

on the graphs ordinate refer to π(z) only). The scaling factor for the density <strong>of</strong> the dumb-bells<br />

is two times smaller than the scaling for water <strong>and</strong> <strong>lipid</strong> densities. The densities refer to water<br />

(w), <strong>lipid</strong> headgroup (h), <strong>lipid</strong> hydrophobic tail-beads excluding the last one (t(1,...,n−1)), last<br />

tail-bead (tn), <strong>and</strong> dumb-bells (db). For the pure bilayer the total density ρtot is also plotted.

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