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computer modeling in molecular biology.pdf

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8 Path Energy M<strong>in</strong>imization 219A further set of methods is based on adapt<strong>in</strong>g a MD simulation from one stateso that the molecule is forced to move towards the state of <strong>in</strong>terest. At least threetechniques have <strong>in</strong>dependently been proposed. The Contra MD method [33, 341takes a short free MD run from one state. If the run moves “toward” the desiredtarget conformation it is “accepted” but if this is not case the run is restarted withanother set of <strong>in</strong>itial atomic velocities. This process is repeated until the target conformationis reached. The measure of distance between two conformations used isbased on the same coord<strong>in</strong>ates used for the adiabatic mapp<strong>in</strong>g study undertaken <strong>in</strong>the work [33]. Ech-Cherif El-Kettani and Durup [42] work<strong>in</strong>g on a much larger problemtake a more direct approach <strong>in</strong> that the MD run is started with the <strong>in</strong>italvelocities set so that the system moves toward the desired state. The r. m. s. atomicdisplacement of the molecule with respect to the target conformation is monitoreddur<strong>in</strong>g dynamics and the run is halted when this quantity starts to rise. Velocities arethen reset toward the target conformations and the run is restarted. Once aga<strong>in</strong> theprocedure is repeated until the desired conformation is reached. In contrast, Schlitteret al. [43] use a MD simulation from one conformation with the constra<strong>in</strong>t that thedistance to the target should decrease slowly with time. All these methods make theassumption that the best path between two states is reasonably direct which may notbe true (e. g., consider a change where the best route for a molecule to undergo asimple transition of a s<strong>in</strong>gle dihedral angle from 0 to 90 degrees is to go through atransition state at 180 degrees). Furthermore the transition state configuration is notidentified and at best only a “ball park estimate” as to the energy barrier <strong>in</strong>volvedis obta<strong>in</strong>ed. These methods may prove to be useful to provide <strong>in</strong>itial routes to whichfurther optimization can be applied.The most effective method developed to date for reaction path generation <strong>in</strong> largesystems is the Self Penalty Walk (SPW) procedure due to Elber and co-workers[44, 451. A cha<strong>in</strong> of positions is considered between the fixed end po<strong>in</strong>ts. These aresimultaneously energy m<strong>in</strong>imized with the restra<strong>in</strong>t that the distance between adjacentpo<strong>in</strong>ts should be equal. Further restra<strong>in</strong>ts are added to avoid problems causedby rigid body translations and rotations, and to avoid the route fold<strong>in</strong>g back onitself. The method presented here, Path Energy M<strong>in</strong>imization (PEM), is also basedon an optimization of a series of conformations ly<strong>in</strong>g between the fixed end po<strong>in</strong>tsbut has a number of novel features. The method is discussed at length <strong>in</strong> the nextsection.

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