computer modeling in molecular biology.pdf
computer modeling in molecular biology.pdf
computer modeling in molecular biology.pdf
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8 Path Energy M<strong>in</strong>imization 237The results, shown <strong>in</strong> Table 8-3, show that the energy of <strong>in</strong>dividual forms changesby up to 2 kcal/mol but the energy barrier rema<strong>in</strong>s around 7 kcal/mol. The consistencybetween the results us<strong>in</strong>g a different representation for the metal ion is encourag<strong>in</strong>g.8.5 Conclusions : Potential DevelopmentsThe PEM method has been shown to be a robust and powerful technique for f<strong>in</strong>d<strong>in</strong>greaction paths for conformational changes <strong>in</strong> macromolecules. It has advantagesover the SPW method (the only comparable technique), <strong>in</strong> that sampl<strong>in</strong>g is biasedtowards high energy regions of the path (thus ensur<strong>in</strong>g that the transition state islocated), the cont<strong>in</strong>uity of the f<strong>in</strong>al result is assured and that the result is not dependenton the values taken for restra<strong>in</strong>t parameters.The implementation of the PEM method presented here suffers from the problemof computational efficiency. This is <strong>in</strong> part due to the fact that the energy and forcecalculation rout<strong>in</strong>es <strong>in</strong> TIC have not been adjusted for maximum speed, for examplean atom based non-bonded cut-off procedure is used <strong>in</strong>stead of the more efficientgroup based formalism and the code has not been vectorized. The PEM method wasalso designed with robustness rather than efficiency <strong>in</strong> m<strong>in</strong>d, The present proceduretakes a specified number of equally spaced sample conformations between each pairof mov<strong>in</strong>g po<strong>in</strong>ts but this could be changed so that the rout<strong>in</strong>e occasionally adjuststhe spac<strong>in</strong>g to ensure the peak energy position of each <strong>in</strong>terval is sampled.As shown <strong>in</strong> the D-xylose isomerase example, the PEM procedure can convergeto different paths depend<strong>in</strong>g on the start<strong>in</strong>g set of conformations. It would be verydesirable for the method to always locate the path with the lowest peak energy. Thiswould require that the procedure should f<strong>in</strong>d the global m<strong>in</strong>imum of the objectivefunction: a ubiquitous problem [48]. There are two partial solutions: to startm<strong>in</strong>imization from different start<strong>in</strong>g conformations (see below) and simulated anneal<strong>in</strong>g[49]. The <strong>molecular</strong> dynamics simulated anneal<strong>in</strong>g procedure has been applied<strong>in</strong> a variant of SPW method [42] and could be expected to be useful <strong>in</strong> m<strong>in</strong>imiz<strong>in</strong>gthe PEM objective function - allow<strong>in</strong>g the method to avoid be<strong>in</strong>g trapped <strong>in</strong>local m<strong>in</strong>ima.An important potential improvement to the method would be to apply the procedure<strong>in</strong> dihedral angle coord<strong>in</strong>ate space. This would require the <strong>molecular</strong> potentialenergy and force functions be calculable <strong>in</strong> terms of dihedral angle variables [61].This approach would result <strong>in</strong> several advantages compared to the present application<strong>in</strong> Cartesian space. Conformational change is clearly more naturally represented<strong>in</strong> <strong>in</strong>ternal coord<strong>in</strong>ate space because of the division between “soft” (dihedral angles)and “hard” (bond lengths and angles) variables. This would allow the use of fewer