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

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3.4 Surface tension in <strong>lipid</strong> <strong>bilayers</strong> 35<br />

Area compressibility<br />

From the dependence <strong>of</strong> the area per <strong>lipid</strong> on the surface tension, the bilayer area<br />

compressibility can be calculated. The bilayer area compressibility KA is defined as<br />

[77]<br />

Integrating equation 3.21 we have<br />

KA = A<br />

γ = KA ln A<br />

<br />

∂γ<br />

. (3.21)<br />

∂A<br />

Ao<br />

(3.22)<br />

where Ao is the area at the free energy minimum, i.e. at zero surface tension. Exp<strong>and</strong>ing<br />

equation 3.22 around Ao we obtain a linear dependence <strong>of</strong> γ on A<br />

γ ≈ KA<br />

(A − Ao). (3.23)<br />

Ao<br />

In simulation, the area compressibility can be calculated from the above equation,<br />

either by fixing the area <strong>of</strong> the bilayer <strong>and</strong> computing the corresponding surface tension,<br />

or by imposing the surface tension <strong>and</strong> calculating the area. In this study we<br />

use the latter method. If the area is taken as the dependent variable, then, from 3.23,<br />

we have<br />

A = Ao<br />

γ + Ao<br />

(3.24)<br />

KA<br />

To fit the area as function <strong>of</strong> γ using equation 3.24, we used two approaches. The<br />

first one consists in computing the area at different values <strong>of</strong> imposed surface tension,<br />

in the regime were the area dependence on surface tension is linear. We found<br />

the behavior <strong>of</strong> the average projected area per <strong>lipid</strong> to be linear in the applied surface<br />

tension for values <strong>of</strong> the tension in the range γ=[-0.5,1.5]. The second method<br />

consists in considering the spontaneous fluctuations at equilibrium, <strong>of</strong> both the area<br />

<strong>and</strong> the measured surface tension, in a tensionless bilayer, as computed in the histogram<br />

shown in figure 3.6(b). The results <strong>of</strong> both fitting methods are in very good<br />

agreement: in both cases we find KAR 2 c/kBT=20.8 from the slope <strong>of</strong> the fitted lines.<br />

Also, a value <strong>of</strong> 1.66 R 2 c is found as the intercept, which is the same value <strong>of</strong> the area<br />

at zero surface tension, Ao, as directly measured from the simulation at γ = 0.<br />

Using Rc=6.4633 ˚A <strong>and</strong> taking kBT as room temperature, i.e. kBT = 4.14 10 −21 J, we<br />

can convert the area compressibility into physical units, resulting in KA ≈ 210 mN/m.<br />

This value is comparable to the value <strong>of</strong> the compressibility equal to 300 mN/m found<br />

by Lindahl <strong>and</strong> Edholm [77] in atomistic MD simulations <strong>of</strong> <strong>lipid</strong> <strong>bilayers</strong>, <strong>and</strong> to<br />

the values measured by micropipette aspiration experiments which, for saturated<br />

phosphatidylcholine <strong>bilayers</strong> in the fluid phase, are also in the range 230-240 mN/m<br />

[78].

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