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note
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In the AIM formalism, although the total molecular energy is recovered by summing the atomic contributions, the recovery of molecular dipoles is less straightforward. Because the charge is partitioned into atomic basins, each "atom" has a net charge (summing to zero for a neutral molecule) and an atomic dipole representing asymmetry of charge within the atomic basin. To recover a molecular dipole from atomic charges and dipoles, the contribution from the relative positions of the charged nuclear attractors is added to that of the sum of the atomic dipoles (ref 14). When a dipole is induced by a perturbation such as an applied field, or as in our case the change of conformation, there are two possible contributions. The atomic dipoles representing distortion of charge within the basins change. There is also a change in the charge-separation term that includes transfer of charge across the interatomic boundary, changing the amount of charge being separated, and geometry relaxations that change the distance by which charge is separated. The charge-separation contribution to the dipole is directed precisely between the two nuclear attractors, while in general, the atomic dipole contribution can be in any direction.
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