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Additives polarizability

A similar scheme can be exploited to compute the additional polarizability a(—wa wa) in this case the time-dependent problem to solve is determined by the Fock operator in which the external perturbation is the polarization P"" and thus the dipole-like operator to be included is m only. The resulting polarizability is now ... [Pg.245]

Small effects of non-additive polarizability terms, included in the ion-w or w-w potentials, have been observed by Smith and Dang [118] on ion-ion pmf. In fact, the SPC/E potential combined with a simple model for the ion-water interactions (Coulomb-f-LJ) is able to reproduce the pmf obtained with the polarizable potential, within statistical uncertainty of the simulation. Also, orientational effects on water molecules of the first hydration shell are described much the same way by the two types of potential, with minor differences as to the population of bridging water, more pronounced for Cl. ... [Pg.413]

D. The calculations confirm that the negative end of the dipole is towards phosphorus. - The calculated dipole moments of phosphole (1.9 D) and pyrrole (2.0 D) are similar, and, unlike furan, the positive ends of the dipoles are towards the heteroatoms. Dipole moments have been used, in combination with results from other methods of study, to estimate the preferred conformations of the dichloride (179), of the phosphites (180), and of triarylphosphine oxides. The use of dipole moments to aid stereochemical studies of compounds has been reviewed. Additive polarizability parameters should not be used in the calculations, and it has been recommended that data should be obtained from model compounds containing identical environments for the phosphorus atoms. The sensitivity of bond moments to structural changes has been studied perfluoroalkyl groups lower the phosphoryl bond moment, and the P—N bond moment is very sensitive to the valence state of the phosphorus atom. The conformational analyses of phospho-nates, phosphonamides, silyl phosphates, and a number of dioxaphosphori-nans (181) - have been reported. The P—Se bond moment has been estimated to be 1.24 D. The zwitterionic structure (182) was identified by its high dipole... [Pg.267]

To conclude this section, we mention an article [68] that discusses desirable features for next-generation NDDO-based semiempirical methods. Apart from orthogonalization corrections and effective core potentials that are already included in some of the more recent developments (see above) it is proposed that an implicit dispersion term should be added to the Hamiltonian to capture intramolecular dispersion energies in large molecules. It is envisioned that dispersion interactions can be computed self-consistently from an additive polarizability model with some short-range scaling [68]. [Pg.569]

Influence of U.V. Radiation. Above 180 C the values of s and tan 6 rise significantly more rapidly for the u.v.-resistant LEXAN 143 than for either 141 or 145 and in a manner which seems to be independent of frequency [1]. It is postulated that u.v.-protection in the 143 material is conferred by intimate association of the benzotriazole additive with the polymer molecules, and that above 180 C this additive is liberated from the polymer molecules, freeing additional polarizable groups which contribute to the observed increase in 8, 8 and tan 8. [Pg.152]

The induction energy is inlierently non-additive. In fact, the non-additivity is displayed elegantly in a distributed polarizability approach [28]. Non-additive induction energies have been found to stabilize what appear to be highly improbable crystal structures of the alkalme earth halides [57]. [Pg.194]

Figure Bl.2.2. Schematic representation of the polarizability of a diatomic molecule as a fimction of vibrational coordinate. Because the polarizability changes during vibration, Raman scatter will occur in addition to Rayleigh scattering. Figure Bl.2.2. Schematic representation of the polarizability of a diatomic molecule as a fimction of vibrational coordinate. Because the polarizability changes during vibration, Raman scatter will occur in addition to Rayleigh scattering.
Until now, we have discussed the use of additivity schemes to estimate global properties of a molecule such as its mean molecular polarizability, its heat of formation, or its average binding energy to a protein receptor. [Pg.327]

In Section 7.1.2 a method for the calculation of mean molecular polarizability was presented. Mean molecular polarizability can be calculated from additive contributions of the atoms in their various hybridization states in a molecule (see Eq. (6)). Mean molecular polarizability, a, expresses the magnitude of the dipole moment, fi, induced into a molecule imder the influence of an external field, E (Eq. (15))... [Pg.333]

The molecular electronic polarizability is one of the most important descriptors used in QSPR models. Paradoxically, although it is an electronic property, it is often easier to calculate the polarizability by an additive method (see Section 7.1) than quantum mechanically. Ah-initio and DFT methods need very large basis sets before they give accurate polarizabilities. Accurate molecular polarizabilities are available from semi-empirical MO calculations very easily using a modified version of a simple variational technique proposed by Rivail and co-workers [41]. The molecular electronic polarizability correlates quite strongly with the molecular volume, although there are many cases where both descriptors are useful in QSPR models. [Pg.392]

Neither bromine nor ethylene is a polar molecule but both are polarizable and an induced dipole/mduced dipole force causes them to be mutually attracted to each other This induced dipole/mduced dipole attraction sets the stage for Br2 to act as an electrophile Electrons flow from the tt system of ethylene to Br2 causing the weak bromine-bromine bond to break By analogy to the customary mechanisms for electrophilic addition we might represent this as the formation of a carbocation m a bimolecular elementary step... [Pg.257]

This result, called the Clausius-Mosotti equation, gives the relationship between the relative dielectric constant of a substance and its polarizability, and thus enables us to express the latter in terms of measurable quantities. The following additional comments will connect these ideas with the electric field associated with electromagnetic radiation ... [Pg.668]

We define the concentration of fluctuation domains at any instant by the symbol N. In addition, we assume that the polarizability associated with one of these domains differs from the macroscopic average value for the substance... [Pg.679]

Chemical Properties. The chemistry of ketenes is dominated by the strongly electrophilic j/)-hybridi2ed carbon atom and alow energy lowest unoccupied molecular orbital (LUMO). Therefore, ketenes are especially prone to nucleophilic attack at Cl and to [2 + 2] cycloadditions. Less frequent reactions are the so-called ketene iasertion, a special case of addition to substances with strongly polarized or polarizable single bonds (37), and the addition of electrophiles at C2. For a review of addition reactions of ketenes see Reference 8. [Pg.473]

In addition, the potential of the electrode can be varied, resulting in a change in the stmcture of the interface. If no current is passed when the potential of the electrode changes, the electrode is called an ideally polarizable electrode, and can be described using thermodynamics. [Pg.64]

The stereochemistry of chlorination can be explained in similar terms. Chlorine would be expected to be a somewhat poorer bridging group than bromine because it is less polarizable and more resistant to becoming positively charged. Comparison of the data for bromination and chlorination of E- and Z-l-phenylpropene confirms this trend (see Table 6.2). Although anti addition is dominant in bromination, syn addition is slightly preferred... [Pg.362]

Silica gel, per se, is not so frequently used in LC as the reversed phases or the bonded phases, because silica separates substances largely by polar interactions with the silanol groups on the silica surface. In contrast, the reversed and bonded phases separate material largely by interactions with the dispersive components of the solute. As the dispersive character of substances, in general, vary more subtly than does their polar character, the reversed and bonded phases are usually preferred. In addition, silica has a significant solubility in many solvents, particularly aqueous solvents and, thus, silica columns can be less stable than those packed with bonded phases. The analytical procedure can be a little more complex and costly with silica gel columns as, in general, a wider variety of more expensive solvents are required. Reversed and bonded phases utilize blended solvents such as hexane/ethanol, methanol/water or acetonitrile/water mixtures as the mobile phase and, consequently, are considerably more economical. Nevertheless, silica gel has certain areas of application for which it is particularly useful and is very effective for separating polarizable substances such as the polynuclear aromatic hydrocarbons and substances... [Pg.93]


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See also in sourсe #XX -- [ Pg.221 ]




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Additivity rule, dipole polarizabilities

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