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computer modeling in molecular biology.pdf

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6 Theory of Transuort <strong>in</strong> Zon Channels 159Reactant to ProductReactant to Reactant2000 -10001500 1Eg 1000500 1 9 500c0 ;(D 0 :ae-500 1 9 -500- tt0-1000 e -1000-1500-2000-1.2 -0.8 -0.4 0 0.4 0.8 1.2t <strong>in</strong>ps-Q-1500;-;--2000-1.2 -0.8 -0.4 0 0.4 0.8 1.2t <strong>in</strong>ps20001500E1000P3 500eI!00-500L3g -1000Reactant to Product------IEf- C2000150010003 500I 0e9 -500gsL-1000Reactant to Reactant7-1500-1500-2000-1.2 -0.8 -0.4 0 0.4 0.8 1.2t <strong>in</strong>ps-2000-1.2 -0.8 -0.4 0 0.4 0.8 1.2t <strong>in</strong>psFigure 6-7. Typical example of the <strong>in</strong>stantaneous forces act<strong>in</strong>g on Na' ion dur<strong>in</strong>g the reactivetrajectory, reactant to product, and the non-reactive trajectory, reactant to reactant, shown<strong>in</strong> Figure 6-6. The forces exerted by the channel and the two nearest water molecules areshown. The carbonyl forces are not dom<strong>in</strong>ant dur<strong>in</strong>g the cross<strong>in</strong>g event. The dom<strong>in</strong>ant forcescaus<strong>in</strong>g the recross<strong>in</strong>g arise primarily from the nearest carbonyl oxygens.reactive trajectory. Dur<strong>in</strong>g the successful cross<strong>in</strong>g the water forces oscillate rapidlyand are predom<strong>in</strong>ant whereas the channel forces have moderate amplitude. Dur<strong>in</strong>gthe failed cross<strong>in</strong>g the channel forces are much larger while the water forces havesimilar amplitudes than dur<strong>in</strong>g the reactive trajectory, The nearest water molecules

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