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for holo as well as apo forms, but low for distorted conformations which are entropically<br />

unfavorable or which involve interpenetrating domains.<br />

A fitness function containing the above terms can be sketched out on the basis of physical<br />

arguments and adjusted empirically. Binding energy is clearly related to the correctness<br />

of the protein structure. Stability is high for both apo and holo, and further is only<br />

estimated here. The quantity was found to be somewhat noisy and so a weighting factor<br />

was used to reduce its influence. Holm and Sander[35] model the interaction between<br />

domains as quadratic, arguing that under the Lennard-Jones model of van der Waals<br />

interactions this approximation holds over a substantial range. Accordingly, the gyration<br />

radius appears squared. Domain distortion can be thought of in the normal mode basis as<br />

a displacement against an elastic potential, but here is reported in units of RMSD, and so<br />

the weighting factor is entirely empirical. The weighting factors applied to all of the<br />

terms except binding energy are determined below. Minimizing the resulting fitness<br />

function can lead to correct generation and identification of the holo structure for domain<br />

hinge bending proteins given only the apo structure, as we will show. We fitted weights<br />

to each of the terms in the fitness function such as to maximize the method’s performance<br />

for Glutamine Binding Protein, as we will explain in the section of that name.<br />

Method<br />

As mentioned, the method requires the identification of the hinge, rotations based on that<br />

hinge, followed by optional equilibrations and docking runs. The direction of the<br />

243

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