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Fitting the Charges

Because atomic charge is not a quantum mechanical observable, we must use some indirect method to calculate these values. Moreover, since we lack experimental results to guide us, other methods of validating our assignments must be devised. Accurate reproduction of some observable, whether experimentally measured (dipole moment) or determined directly from the wavefunction (electrostatic potential, molecular moments, etc.), increases our confidence in the reliability of the assigned charges. [Pg.4]

The molecular electrostatic potential at a point in space r can be calculated from the charge distribution using ° [Pg.4]

This can be written in the linear-combination-of-atomic-orbitals molecular orbital (LCAO-MO) formalism as follows [Pg.4]

Kollman suggested that the electron density could be partitioned into a set of monopole charges based on the electrostatic potential. At the same time, Momany showed that a set of monopole charges could be fit to the electrostatic potential. Atom-centered point charges that best fit the overall MEP were determined by iterative minimization of the following function  [Pg.5]

The constraint of reproducing the overall charge on the species is placed on the assignment of the point charges. [Pg.5]


The auxiliary basis sets to fit the charge density P and the exchange-correlation potential U are defined as... [Pg.262]

One should keep in mind that the procedure to fit the charges to nuclei only is completely arbitrary. One could just as well fit the EP to charges centered at bond midpoints or anywhere else. In fact, a superior fit could be obtained by optimizing the position of the charges along with the charges themselves. [Pg.195]

The first option is to fit the charge density. The fitted density, p(r), given by... [Pg.227]

The solvent dielectric constant, ionic strength and temperature are chosen to fit the conditions of the experimental studies. The protein dielectric constant is assigned some small value, e.g. 4. The PB calculations are currently carried out with the atomic charges and radii of the PARSE parameter set, developed by Honig and coworkers [17] or that for CHARMM [12]. The PARSE parameter set... [Pg.182]

Fig. 7. The field-dependence of the charge-generation efficiency of a 2.0- lm thick (0) a l.l-).tm thick ( ), and 1.8-).tm thick (A) fuUerene/PMPS film obtained with positive charging and 340-nm irradiation (A). The soHd lines are calculated from the Onsager model. The best-fit curve is obtained with Tq = 2.7 nm and = 0.85. Also plotted is the charge-generation efficiency of a fuUerene/PVK film (+) obtained with positive charging and 340-nm irradiation (B). The soHd lines are calculated from the Onsager model. The best-fit curve is obtained with = 1.9 nm and = 0.9 (13). Fig. 7. The field-dependence of the charge-generation efficiency of a 2.0- lm thick (0) a l.l-).tm thick ( ), and 1.8-).tm thick (A) fuUerene/PMPS film obtained with positive charging and 340-nm irradiation (A). The soHd lines are calculated from the Onsager model. The best-fit curve is obtained with Tq = 2.7 nm and = 0.85. Also plotted is the charge-generation efficiency of a fuUerene/PVK film (+) obtained with positive charging and 340-nm irradiation (B). The soHd lines are calculated from the Onsager model. The best-fit curve is obtained with = 1.9 nm and = 0.9 (13).
Experimental Values of Charge-Generation Efficiencies. In this section the charge-generation efficiencies of many polymeric photoconductors are compared (Table 3). When the experimental data has been fitted to the Onsager model, the initial electron—hole separation distance,... [Pg.416]

An acid egg, or blowcase, consists of an egg-shaped container which can be filled with a charge of liquid that is to be pumped. This container is fitted with an inlet pipe for the charge, an outlet pipe for the discharge, and a pipe for the admission of compressed air or gas, as illustrated in Fig. 10-58. Pressure of air or gas on the surface of the liquid forces it out of the discharge pipe. Such pumps can be hand-operated or arranged for semiautomatic or automatic operation. [Pg.913]

In general, the reaction between a phenol and an aldehyde is classified as an electrophilic aromatic substitution, though some researchers have classed it as a nucleophilic substitution (Sn2) on aldehyde [84]. These mechanisms are probably indistinguishable on the basis of kinetics, though the charge-dispersed sp carbon structure of phenate does not fit our normal concept of a good nucleophile. In phenol-formaldehyde resins, the observed hydroxymethylation kinetics are second-order, first-order in phenol and first-order in formaldehyde. [Pg.883]

Her workers to fit the exchange-correlation potential and the charge density (in the Coulomb potential) to a linear combination of Gaussian-typc functions. [Pg.43]

The two-stage electrostatic precipitators used in light-industry applications are compact devices which can be fitted into the ventilation system. These air cleaners are normally used to clean air from dusts, smokes, and fumes in industrial workplaces. The basic features of these devices are the separate sections for particle charging and collection. The charging section consists of thin metal wires installed between grounded metal plates. The distance... [Pg.1230]


See other pages where Fitting the Charges is mentioned: [Pg.164]    [Pg.187]    [Pg.168]    [Pg.173]    [Pg.339]    [Pg.462]    [Pg.5]    [Pg.37]    [Pg.132]    [Pg.253]    [Pg.356]    [Pg.164]    [Pg.187]    [Pg.168]    [Pg.173]    [Pg.339]    [Pg.462]    [Pg.5]    [Pg.37]    [Pg.132]    [Pg.253]    [Pg.356]    [Pg.209]    [Pg.352]    [Pg.88]    [Pg.208]    [Pg.208]    [Pg.209]    [Pg.209]    [Pg.210]    [Pg.237]    [Pg.238]    [Pg.588]    [Pg.251]    [Pg.580]    [Pg.385]    [Pg.86]    [Pg.415]    [Pg.415]    [Pg.108]    [Pg.327]    [Pg.290]    [Pg.195]    [Pg.1650]    [Pg.21]    [Pg.29]    [Pg.397]    [Pg.80]    [Pg.157]    [Pg.211]    [Pg.372]   


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