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Oscillation Model evaluate

Note that in a sudden transition, eq. 3 is a more general relation than the Golden role (see, e.g., reference 15). In that circumstance the Golden rule appears as a special case of the FC factor, corresponding to small V and the applicability of perturbation theory. In order to evaluate the FC factor, Berry used the dressed oscillator model which, in principle, coincides with the previously described quasi-diatomic method. [Pg.99]

A theoretical evaluation of the aromaticity of the pyrones pyromeconic acid, maltol, and ethylmaltol along with their anions and cations was carried out at several levels (Hartree-Fock, SVWN, B3LYP, and B1LYP) using the 6-311++G(d,p) basis set <2005JP0250>. The relative aromaticity of these compounds was evaluated by harmonic oscillator model of aromaticity (HOMA), nucleus-independent chemical shifts (NICSs), and /6 indexes and decreases in the order cation > neutral molecule > anion. [Pg.347]

Since DFT calculations are in principle only applicable for the electronic ground state, they cannot be used in order to describe electronic excitations. Still it is possible to treat electronic exciations from first principles by either using quantum chemistry methods [114] or time-dependent density-functional theory (TDDFT) [115,116], First attempts have been done in order to calculate the chemicurrent created by an atom incident on a metal surface based on time-dependent density functional theory [117, 118]. In this approach, three independent steps are preformed. First, a conventional Kohn-Sham DFT calculation is performed in order to evaluate the ground state potential energy surface. Then, the resulting Kohn-Sham states are used in the framework of time-dependent DFT in order to obtain a position dependent friction coefficient. Finally, this friction coefficient is used in a forced oscillator model in which the probability density of electron-hole pair excitations caused by the classical motion of the incident atom is estimated. [Pg.21]

Several aspects of aromaticity have been studied <2002JOC1333> using statistical analyses of quantitative definitions of aromaticity. ASEs, REs, magnetic susceptibility exaltation (A), nucleus-independent chemical shift (NIGS), the harmonic oscillator model of aromaticity (HOMA), (/j) and (Aj), evaluated for a set of 75 five-membered 7t-electron systems and a set of 30 ring-monosubstituted compounds (aromatic, nonaromatic, and antiaromatic systems) revealed statistically significant correlations between the various aromaticity criteria, provided the whole set of compounds is used. The data in Table 9 have been found for arsole (AsH) 1 (E = As, R = H), its anion (As ), and protonated species (AsH2 ). [Pg.1161]

The harmonic oscillator model enables measurement of the bond force constant through vibrational spectroscopy as follows. The measured frequency of the radiation absorbed is the same as the vibrational frequency of the molecule. The reduced mass is calculated for the molecule, and the force constant is evaluated as k =... [Pg.161]

By resolution of both light-absorption and CD bands of ARN and FAD and by the use of both experimental and theoretical values for transition moments, conformations of the relevant molecules were deduced. However, because of difficulties in accurate assignment and determination of the various transition moments and because of the limitations inherent in calculations using the coupled oscillator model and dipole-dipole interaction potentials, only a qualitative picture of the conformations involved could be expected (12). Generally, reciprocal relations between known transitions were taken as evidence for juxtaposition of the corresponding chromophores (12). The optical data obtained for coenzymes or their model compounds may be utilized in favorable cases for estimating structural features in the bound state, in which the interactions with the protein environment will also have to be evaluated. [Pg.107]

Note added in proof In view of the failure of the harmonic oscillator model to account for the observed rate of activation in unimolecular dissociation reactions (the dissociation lag problem) these calculations have been repeated for a Morse anharmonic oscillator with transition between nearest and next-nearest neighbor levels [S. K. Kim, /. Chem. Phys. (to be published)]. The numerical evaluation of the analytical results obtained by Kim has not yet been carried out. From the results obtained by us and our co-workers [Barley, Montroll, Rubin, and Shuler, /. Chem. Phys. in press)] on the relaxation of vibrational nonequilibrium distributions of a system of Morse anharmonic oscillators it seems clear, however, that the anharmonic oscillator model with weak interactions (i.e., adiabatic perturbation type matrix elements) does not constitute much of an improvement on the harmonic oscillator model in giving the observed rates of activation. The answer to tliis problem would seem to lie in a recalculation of the collisional matrix elements for translational-vibrational energy exchange which takes account of the strong interactions in highly energetic collisions which can lead to direct dissociation. [Pg.392]

As already mentioned, quantitative estimation of the entropy of a liquid is astonishingly difficult. For the solid state, one can evaluate the entropy by assuming a harmonic oscillator model for each mode of vibration of the atoms/molecules. The... [Pg.295]

To evaluate the oscillation model, the components of its equations ought to be measured experimentally. Some parameters such as, and N can be easily estimated. However, for some internal parameters such as, yam-to-yam friction coefCfcient and normal load in the crossing points, there are no empirical approaches. These parameters are related to the internal mechanical properties of the plain woven fabrics, have not been meastrred directly yet. As an alternative, the force balance model, which has been introduced by Valizadeh et al, is errrployed to estirrtate these parameters [10]. [Pg.134]

Hasegawa, T., Nishijo, J., Umemura, J. and Theiss, W. (2001) Simultaneous evaluation of molecular-orientation and optical parameters in ultrathin films by oscillators-model simulation and infrared external reflection spectrometry. J. Phys. Chem. B, 105, 11178-11185. [Pg.139]

Visco-elastic substances can be described with the spring/shock-absorber model of Kevin and Voigt, and have phase displacements of 0° to 90°. In analogy to other time dependent processes in physics, the oscillation tests are evaluated with complex arithmetics. Obtained are the complex quantities ... [Pg.417]

To evaluate model, we focus on the experimentally observed metabolic state of the pathway. However, in the case of sustained oscillations, the (unstable) steady state cannot be observed directly. We thus approximate the metabolic state by the average observed concentration and flux values, as reported in Refs. [101, 126], See Table VII for numeric values. [Pg.203]

Evaluating the structural kinetic model, we first consider the possibility of sustained oscillations. Starting with the simplest scenario, all saturation parameters are set to unity, corresponding to bilinear mass-action kinetics and... [Pg.204]

The relaxation spectrum greatly influences the behaviour observed in experiments. As an example of this we can consider how the relaxation spectrum affects the storage and loss moduli. To evaluate this we need to change the kernel to that for a Maxwell model in oscillation and replace the experimental time by oscillation frequency ... [Pg.118]

When the results of a molecular dynamics study are being judged, the question, Is the potential realistic is often asked. This can be the incorrect approach to evaluating the validity of a computer simulation. The appropriate question to be addressed should be, Ts the potential used appropriate for the phenomena being modeled . In the same vein, it is common for a potential developed to model one property of a system to be arbitrarily extended to phenomena for which it may be inappropriate. In this way, interaction potentials are often misjudged. For example, pair potentials with tails that mimic the oscillations present in an electron gas due to ion cores can be used to understand the properties of bulk metals. It is obvious that these potentials, however, would not realistically describe the interaction between three metal atoms, where an electron gas is not well defined. It is the rare interaction potential which works well for all properties of a particular system and so one needs to understand why a particular potential works well for a given property. [Pg.286]

Stewart s conclusion underscores the need for short-wavelength, low-temperature studies, if very high accuracy electrostatic properties are to be evaluated by Fourier summation. But, as pointed out by Hansen (1993), the convergence can be improved if the spherical atoms subtracted out are modified by the k values obtained with the multipole model. Failure to do this causes pronounced oscillations in the deformation density near the nuclei. For the binuclear manganese complex ( -dioxo)Mn(III)Mn(IV)(2,2 -bipyridyl)4, convergence of the electrostatic potential at the Mn nucleus is reached at 0.7 A" as checked by the inclusion of higher-order data (Frost-Jensen et al. 1995). [Pg.173]


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