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interpenetrating domains. This problem led to the introduction of the next two quantities<br />

into the fitness function.<br />

Domain distortion is a measure we devised to represent the degree to which domains 1<br />

and 2 differed structurally from their conformations in the starting structure. As was<br />

observed by Schlauderer et al[121] domain structure is typically conserved during<br />

domain hinge bending motion, even across structures of substantially different sequence;<br />

in fact the definition of domain hinge bending requires this[8,9]. This quantity is zero for<br />

the starting structure and so cannot be used alone for prediction; the point is instead to<br />

exclude from consideration generated structures with interpenetrating or otherwise<br />

improbably deformed domains.<br />

Free energy of folding, or stability, can be used to discriminate energetically feasible<br />

conformers from those with unnatural orientation or excessively interpenetration of<br />

domains. However since a wide variety of conformers, including both the holo and the<br />

apo, are stable, this measure alone cannot find the holo structure in an ensemble. The<br />

point is again to exclude unphysical structures.<br />

These four terms together suggest a physical model of ligand binding in domain hinge<br />

bending proteins. Binding energy is lowest in the apo structure because the former<br />

stabilizes the latter. Radius of gyration is minimized as the solvent-filled volume of the<br />

cleft diminishes during closure; this position is stabilized by inter-domain and domain-<br />

ligand contacts, including many van der Waals interactions which are approximately<br />

quadratic as we will discuss. Domain distortion is disfavored because by definition<br />

structural domains are are already in their stable conformation[8,9,112]. Stability is high<br />

242

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