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Biophysical studies of membrane proteins/peptides. Interaction with ...

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INTRODUCTION: LIPID-PROTEIN INTERACTIONS<br />

excluded-volume interactions between headgroups. The resulting free-energy pr<strong>of</strong>ile for<br />

lipid-protein mismatch was nearly symmetrical about the point <strong>of</strong> hydrophobic<br />

matching, and the lipid perturbation energy F (in units <strong>of</strong> kT per Å 2 <strong>of</strong> protein<br />

circumference) is described by (Ben-Shaul, 1995):<br />

F<br />

( ) 2<br />

= 0,37<br />

+ 0,005 ⋅ d P<br />

− d L<br />

2.3<br />

This model assumed concentration <strong>of</strong> the hydrophobic mismatch perturbation on the<br />

first shell <strong>of</strong> lipids around the protein (see 2.7). For a hydrophobic mismatch <strong>of</strong> 7 Å and<br />

assuming that each lipid adjacent to the protein should occupy at least 4 Å 2 <strong>of</strong> the<br />

protein perimeter, the free-energy for lipid-protein interaction would increase by 3.6 kJ<br />

mol -1 . This change in lipid-protein interaction energy corresponds to a decrease factor in<br />

lipid-protein binding constant <strong>of</strong> 4.3. If propagation <strong>of</strong> perturbation spreaded to the<br />

more external shells, the effects <strong>of</strong> hydrophobic mismatch on the adjacent lipid<br />

molecules would be decreased. For example, if effects were averaged over three shells<br />

<strong>of</strong> lipids, the change in binding constant would decrease by a factor <strong>of</strong> 1.6 (Mall et al.,<br />

2002). Alternative models for treating hydrophobic mismatch came to very similar<br />

conclusions regarding interaction energies (Nielsen et al., 1998; Mouritsen and Bloom,<br />

1993).<br />

Energies <strong>of</strong> this magnitude are sufficient to induce changes not only in the<br />

interacting lipid molecules but in the protein itself. Experimental <strong>studies</strong> allowed to<br />

conclude that β-barrel <strong>proteins</strong> are not easily susceptible to structural/conformational<br />

changes due to hydrophobic mismatch and the energetic penalty for protein-lipid<br />

interaction was only affecting lipid structure (O´Keeffe et al, 2000). However, in the<br />

cases <strong>of</strong> alpha-helical TM <strong>proteins</strong> such as the potassium channel KcsA, and the<br />

mechanosensitive channel MscL, the experimentally obtained dependence <strong>of</strong> binding<br />

constants on the extent <strong>of</strong> hydrophobic mismatch was smaller than expected<br />

(Williamson et al., 2002; Powl et al., 2003). This was rationalized as due to the smaller<br />

rigidity <strong>of</strong> the α-helical <strong>proteins</strong> that makes them susceptible to distortion when<br />

hydrophobic mismatch was present and therefore create an additional degree <strong>of</strong> freedom<br />

for relaxation <strong>of</strong> lipid-protein hydrophobic mismatch. Distortion <strong>of</strong> α-helical <strong>membrane</strong><br />

<strong>proteins</strong> by hydrophobic mismatch is supported by the observation that the activities <strong>of</strong><br />

33

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