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distorted domains, and does not resemble the holo. The inclusion of the domain<br />

distortion and stability terms counters this problem. The gyration radius appears squared<br />

for the physical reasons metioned earlier and to strongly penalize structures that minimize<br />

docked energy but which bind the ligand by forming a new cleft not observed<br />

experimentally, e.g. by pinching shut the region behind the hinge. In the latter situation a<br />

structure is seen that is much like a clam opened to a very wide angle.<br />

The structure with highest stability, inset 5.3.g, is quite close to the starting structure.<br />

This should not be surprising, since such structures have gone through a minimum of<br />

structural manipulation and so have low steric strain. Stability is another measure whose<br />

point is not to exclusively pinpoint the predicted holo structure, but rather to exclude<br />

from consideration structures which minimize docked energy but which have<br />

entropically or entalphically unfavorable conformations.<br />

Based on these considerations we parameterized the fitness function.<br />

fitness_function = (docked_energy +foldx_energy/10 + gyration_radius 2 /10 + D3RMSD_aligned + D1RMSD_aligned)<br />

The stability or foldx_energy term was noisy and favored the apo structure, therefore we<br />

reduced it by a factor of<br />

1<br />

, which still gave us the ability to weed out unphysical<br />

10<br />

conformations. Similarly the gyration radius term too strongly favored interpenetrating<br />

domains and was ! reduced by the same factor, which still let it retain its ability to weed<br />

out excessively-open conformations. D3RMSD_aligned is the RMSD of domain 3 of the<br />

256

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