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Intermolecular potentials dispersion energy

Figures 5-2 and 5-3. First, the dispersed emission from the cluster Figures 5-2 and 5-3. First, the dispersed emission from the cluster <F contains a good deal of van der Waals mode intensity due to the change in Franck-Condon factor between the two clusters. The difference in Franck-Condon factors probably arises because the Ar/aniline and CFJ4/aniline intermolecular potentials are somewhat different. Second, excitation of the 6a1 state yields only (F and 0° emission with much more intensity in the cluster emission. This suggests that now IVR is fast, VP is slow, and that the cluster binding energy is close to 494 cm-1. Third, emission from the cluster is now hot in that the 0 features are quite broad. The CH4 cluster emission at 6a1 excitation is broad, whereas the Ar cluster emission is sharp due to the difference in Franck-Condon factors for the two clusters.
The parametrization procedure that we have opted for in the most recent works is as follows (1) Compute the intermolecular dynamic correlation energy for the ground state with a second-order Mpller-Plesset (MP2) expression that only contains the intermolecular part and which uses monomer orbitals. Fit the dispersion parameters to this potential. To aid in the distribution of the parameters, a version of the exchange-hole method by Becke and Johnson is sometimes used [154,155], Becke and Johnson show that the molecular dispersion coefficient can be obtained fairly well by a relation that involves the static polarizability and the exchange-hole dipole moment ... [Pg.233]

The method used here for considering conformal solution models for fluids with molecular anisotropies is based on the method used by Smith (4) for treating isotropic one-fluid conformal solution methods as a class of perturbation methods. The objective of the method is to closely approximate the properties of a mixture by calculating the properties of a hypothetical pure reference fluid. The characterization parameters (in this case, intermolecular potential parameters) of the reference fluid are chosen to be functions of composition (i.e., mole fractions) and the characterization parameters for the various possible molecular pair interactions (like-like and unlike-unlike). In principle, all molecular anisotropies (dipole-dipole, quadrupole-quadrupole, dipole-quadrupole, and higher multipole interactions, as well as overlap and dispersion interactions ) can be included in the method. Here, the various molecular anisotropies are lumped into a single term, so that the intermolecular potential energy uy(ri2, on, a>2) between Molecules 1 and 2 of Species i and / can be written in the form... [Pg.134]


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Dispersion potential

Energy dispersal

Energy dispersive

Intermolecular potential

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