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. 2007 Jul 13;93(9):3015–3025. doi: 10.1529/biophysj.107.112086

FIGURE 4.

FIGURE 4

(a) Two-dimensional PMF plot at T = 300 K for the Aβ16–20m inhibitor-Aβ16–22 peptide dimer. The free energy is plotted in units of kJ/mol versus number of interpeptide Cα contacts (x axis) and the cosine of θ, the angle between the two peptides, defined as the angle between the vectors connecting Cα atoms of residues 17 and 19 in the Aβ16–20m inhibitor and residues 18–20 in the Aβ16–22 peptide. The boxes denote the region of phase space representing the lowest energy basins in which conformational clustering was performed. (b and c) The resulting representative structures from the most populated clusters within these basins are shown on the right. Methyl groups are shown as gray spheres, backbone interpeptide hydrogen bonds are shown as dotted lines, and the N-terminus of each strand is highlighted in orange for the Aβ16–20m inhibitor and in violet for the Aβ16–22 peptide. (d) Two-dimensional PMF plot for the trimer consisting of two Aβ16–20m inhibitors and one Aβ16–22 peptide. The free energy is plotted in units of kJ/mol versus number of Aβ16–20m inhibitor-Aβ16–20m inhibitor Cα contacts (x axis) and the total number of Aβ16–22 peptide-Aβ16–20m inhibitor contacts. The box denotes the region of phase space representing the lowest energy basin in which conformational clustering was performed. (eg) The resulting representative structures from the three most populated clusters within this basin are shown on the right.