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computer modeling in molecular biology.pdf

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152 Benoit RouxOne advantage of this formulation is that the mean force can be decomposed l<strong>in</strong>early<strong>in</strong>to a sum of contributions, e.g.,(6-22)and the l<strong>in</strong>earity, preserved by the <strong>in</strong>tegral of the mean force along the reaction coord<strong>in</strong>ate,allows to determ<strong>in</strong>e the contribution Wa(x) of any <strong>in</strong>teraction term to thepotential of mean force,(6-23)with(6-24)This method can be very useful <strong>in</strong> f<strong>in</strong>d<strong>in</strong>g the contribution of the solvent moleculesor specific residues to the free energy profile. The total potential of mean force canbe computed equivalently with the free energy simulation technique, via Eq. (6-17).However, the <strong>in</strong>tegrated mean force decomposition can only be obta<strong>in</strong>ed us<strong>in</strong>gEqs. (6-22), (6-23) and (6-24).The free energy simulation technique is computationally <strong>in</strong>tensive, i. e., to reachconvergence and obta<strong>in</strong> accurate results it is necessary to generate long trajectorieswith the ion constra<strong>in</strong>ed at various positions along the x-axis. For this reason it isof <strong>in</strong>terest to use a system with as small a number of atoms as possible. To avoidthe large number of water molecules necessary to solvate the mouth of the channel,the potential of mean force was calculated for Na’ ion along the axis of a periodic(L, D) poly-alan<strong>in</strong>e P-helix. Such a periodic helix is appropriate for <strong>in</strong>vestigat<strong>in</strong>g thes<strong>in</strong>gle file translocation of the ion and its neighbor<strong>in</strong>g waters <strong>in</strong> the <strong>in</strong>terior of thechannel where end effects and sidecha<strong>in</strong>s are expected to play a secondary role.Moreover, this choice provides a test of the methodology s<strong>in</strong>ce any deviation fromperiodicity of the average properties <strong>in</strong>dicates a lack of convergence <strong>in</strong> virtue of thehelix symmetry.The periodic helix structure was first ref<strong>in</strong>ed <strong>in</strong> the absence of any ion and solventmolecules. The helical parameters, the rise and the rotation angle per (LAla, D-Ala)unit, were optimized by energy m<strong>in</strong>imization with the ABNR algorithm [65]. It wasfound that the optimum rise per unit, hL, is 0.155 nm and the optimum turn perunit, 0, is 114.4 degrees, yield<strong>in</strong>g 6.29 residues per turn; this value is similar to thatof the Urry helix model (6.3) [30]. The total number of particles is 229. The fundamentalunit, treated with periodic boundary conditions to avoid end effects (imagesof the system are repeated along the helix axis), <strong>in</strong>cludes 34 alan<strong>in</strong>e residues,

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