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location graph should have minima at locations that coincide with flexible hinges<br />

between domains. We will explain these terms and methodology in detail.<br />

We start with an energy minimization step, to relieve any close contacts or unnatural<br />

bond lengths or angles in the undivided chain which would bias the results. For this we<br />

use TINKER’s minimize routine with the OPLS-All Atom force field and the Ooi-<br />

Scheraga Solvent Accessible Surface Area (SASA) continuum solvation free energy<br />

term. For each iteration of the predictor, we introduce a cut between residues i - 1 and i.<br />

This divides the protein into two fragments, numbered 1 and 2 (Figure 3.1). Fragment 1<br />

is a polypeptide containing residues 1 to i - 1, and fragment 2 is another polypeptide<br />

containing residues i to N, We use these fragments in an energetic calculation as follows.<br />

We define E C as the single point energy of the complete (undivided) protein. This<br />

includes bonded and non-bonded interactions. In the energy evaluation step we again use<br />

the OPLS-All Atom force field with the SASA implicit solvent model. The energy<br />

reported consists of two parts: the in vacuo potential energy of the molecule, and the free<br />

energy of solvation, computed using the implicit solvent model, Note that this step will<br />

change in the second variant of FlexOracle.<br />

For each choice of cut location i, we compute fragment single point energies ( )<br />

and E frag ( ) . We argue that ! E(i)<br />

= ( )<br />

2 i<br />

E frag 1 i + 2 ( i)<br />

112<br />

E frag 1 i<br />

E frag - E C is related to the energy<br />

change associated with hinge motion about the selected hinge, as follows.

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