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crc press - E-Lib FK UWKS

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

and hydrophilicity values at all the grid nodes was calculated. The hydrophobic and<br />

hydrophilic MHP surfaces were then drawn by joining the isopotential values.<br />

9.3 RESULTS<br />

9.3.1 EFFICIENCY OF MONTE CARLO METHOD APPLIED TO SHORT PEPTIDES<br />

AND MEMBRANE PROTEINS<br />

9.3.1.1 Hydrophobic Peptides<br />

Different peptides have already been studied in order to evaluate the Monte Carlo<br />

method by comparison with known experimental data. Different amphipathic,<br />

transmembrane 31 and tilted peptides 55 have been analyzed in this goal.<br />

18A is a synthetic amphipathic peptide shown to be α-helical and adsorbed at<br />

the water–lipid interface. 56 In Figure 9.5, the restraint envelope is a function of the<br />

peptide mass center penetration and axis tilt with respect to the membrane surface.<br />

In its energy minimum position, the peptide is at the surface of the model bilayer.<br />

For the 18A peptide, the energy minimum is reached when the peptide is in membrane<br />

at about 16 Å of the bilayer center with a tilt of 10°, the position varies between<br />

14-18 Å and 0-20° of angle of insertion, demonstrating that the peptide finds its<br />

local minimum in a position parallel to the interface, which corresponds to a perfectly<br />

amphipathic structure.<br />

The M2δ peptide is a transmembrane α-helix present in the acetylcholine receptor<br />

that can induce the lysis of red blood cells. 57 The peptide is biamphipathic and,<br />

in the presence of a bilayer, it stands almost perpendicularly (around 70°) to the<br />

plane in a transmembrane configuration. 31<br />

The fusion peptide SIV (simian immunodeficiency virus) was among the first<br />

tilted peptides described by molecular modeling (Figure 9.5.C). Tilted peptides have<br />

10 to 20 residues and a peculiar hydrophobicity profile. When analyzed in a helix<br />

FIGURE 9.5 (opposite) The different plots correspond to the peptides 18A (A), M2δ (B),<br />

and SIV (C). IMPALA simulations are shown as 3D plots of the restraint energy vs. the<br />

penetration of the peptide mass center and vs. the angle of insertion of a reference vector.<br />

The reference vector is defined by 2 atoms of a helix or a strand, and the angle of this vector<br />

with the XY plane is the index of the peptide orientation in the bilayer. The protein mass<br />

center penetration in angstroms is plotted on the X axis (0 is the bilayer center); the Y axis<br />

is the angle in degrees of the reference vector. The restraint values are plotted along the Z<br />

axis. The energy minimum zones (light gray) locate the most favorable positions of the<br />

peptides. The 3D envelopes are calculated as follows: a 2D grid using as X axis the position<br />

of the molecule mass center between –15 and 15 Å, by steps of 0.5 Å, and along the Y axis,<br />

the angle of the helix with respect to the plane of the bilayer by steps of 3°. Next, for each<br />

grid knot, the minimal energy restraint is plotted. Data are extracted from the Pex2dstat files.<br />

The ribbon picture of the most stable conformation of each peptide is shown in the model<br />

membrane of IMPALA. The dotted line is the center of the bilayer (Z = 0 Å) and the black<br />

line defines where the polar heads of lipids start (z = ±13.5 Å). The gray line is the water–lipid<br />

interface (z = ±18 Å).

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