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crc press - E-Lib FK UWKS

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214 Cell-Penetrating Peptides: Processes and Applications<br />

E<br />

(top)<br />

(bottom)<br />

Total Restraints (kJ/mol Å 2 )<br />

FIGURE 9.9 (continued)<br />

pAntp (inner leaflet charge: -0.02)<br />

Mass Center Penetration (Å)<br />

core of the bilayer. The lipid perturbation restraint is similar to that calculated for<br />

the first helix and for the full-length homeodomain.<br />

Finally, our simulations predict that, with such a charge distribution, the penetratin<br />

peptide may cross the bilayer due to the influence of membrane charges. This<br />

restraint is indeed greatly favorable during the bilayer crossing simulation. Furthermore,<br />

the evolution of the hydrophobic restraint suggests that the helix hydrophobic<br />

properties would not allow crossing the bilayer hydrophobic core in the absence of<br />

the superficial charge density located at the internal leaflet. However, although the<br />

charge restraint becomes unfavorable from –10 Å, the hydrophobic restraint, in turn,<br />

becomes favorable, and allows the mass center of the third helix to stabilize at –13 Å,<br />

forming a 3° angle with the bilayer plan. The discontinuous course during crossing<br />

(indicated by dots, Figure 9.9E, top) suggests that the crossing is very rapid. Lipid<br />

perturbation restraint stays at the same level as for the previous simulations (8<br />

kJ/mol.Å 2 ), indicating that the crossing has no major destabilizing effects on the<br />

Angle(°)

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