Vibrational models for

Fig. 19. Experimental NMRD profiles and data calculated using classical vibration model for aqueous Ni(II). Thin line SBM thick line general theory. Reproduced with permission from Kruk, D. Kowalewski, J. J. Chem. Phys. 2002,116,4079-4086. Copyright 2002 American Institute of Physics.

Figure 11.3. Temperature dependence of the primary hydrogen isotope effect calculated using a 9-atom vibrational model for hydrogen transfer (model HHIE3 [37] with simple stretch-stretch coupling to generate a reaction-coordinate frequency). Triangles mark calculated results for models with a reaction-coordinate frequency for H transfer of 9841 cm including the truncated Bell tunnel correction [6, 22]. The circles show results for models with a sufficiently low reaction-coordinate frequency (901 cm ) to make the...

The available data, including ab initio molecular orbital calculations of the transition-state structures, indicate that a vibrator model for the transition state accounts for the k E, J) curves. Both the ab initio calculations and the experimental rate constants indicate that the H loss transition state has a slightly tight transition state. Figure 7.14 shows how the rates for reactions (7.25(a))-(7.25(c)) vary with J. Note that the rate constants for H loss channel decrease much more rapidly with J because... 

Winterstein, S.R., 1988. Nonlinear vibration models for extremes and fatigue. Journal of Eng. Meek, ASCE, 114, 1772-1790. 

Barrio, R., E.L. CastUUo-Alvarado, and E.L. Galeener. 1991. Structural and vibrational model for vitreous boron oxide. Phys. Rev. B 44 7313-7320. 

Dynamic models for ionic lattices recognize explicitly the force constants between ions and their polarization. In shell models, the ions are represented as a shell and a core, coupled by a spring (see Refs. 57-59), and parameters are evaluated by matching bulk elastic and dielectric properties. Application of these models to the surface region has allowed calculation of surface vibrational modes [60] and LEED patterns [61-63] (see Section VIII-2). 

Morse [119] introduced a potential energy model for tire vibrations of bound molecules... 

Zhu L, Chen W, Hase W L and Kaiser E W 1993 Comparison of models for treating angular momentum in RRKM calculations with vibrator transition states. Pressure and temperature dependence of CI+C2H2 association J. Phys. Chem. 97 311-22... 

Troe J 1995 Simplified models for anharmonic numbers and densities of vibrational states. I. Application to NO2 and Chem. Phys. 190 381-92... 

Figure A3.13.15. Master equation model for IVR in highly excited The left-hand side shows the quantum levels of the reactive CC oscillator. The right-hand side shows the levels with a high density of states from the remaining 17 vibrational (and torsional) degrees of freedom (from [38]).

Zhang J Z H 1999 The semirigid vibrating rotor target model for quantum polyatomic reaction dynamics J. 

The homonuclear rare gas pairs are of special interest as models for intennolecular forces, but they are quite difficult to study spectroscopically. They have no microwave or infrared spectmm. However, their vibration-rotation energy levels can be detennined from their electronic absorjDtion spectra, which he in the vacuum ultraviolet (VUV) region of the spectmm. In the most recent work, Hennan et al [24] have measured vibrational and rotational frequencies to great precision. In the case of Ar-Ar, the results have been incoriDorated into a multiproperty analysis by Aziz [25] to develop a highly accurate pair potential. 

For the model Hamiltonian used in this study it was assumed that bond stretching satisfactorily describes all internal vibrational motions for a system of linear molecules and the split parts of the Hamiltonian were of the form... 

The harmonie oseillator energies and wavefunetions eomprise the simplest reasonable model for vibrational motion. Vibrations of a polyatomie moleeule are often eharaeterized in terms of individual bond-stretehing and angle-bending motions eaeh of whieh is, in turn, approximated harmonieally. This results in a total vibrational wavefunetion that is written as a produet of funetions one for eaeh of the vibrational eoordinates. 

The examples examined earlier in this Chapter and those given in the Exereises and Problems serve as useful models for ehemieally important phenomena eleetronie motion in polyenes, in solids, and in atoms as well as vibrational and rotational motions. Their study thus far has served two purposes it allowed the reader to gain some familiarity with applieations of quantum meehanies and it introdueed models that play eentral roles in mueh of ehemistry. Their study now is designed to illustrate how the above seven rules of quantum meehanies relate to experimental reality. 

This pieture is that deseribed by the BO approximation. Of eourse, one should expeet large eorreetions to sueh a model for eleetronie states in whieh loosely held eleetrons exist. For example, in moleeular Rydberg states and in anions, where the outer valenee eleetrons are bound by a fraetion of an eleetron volt, the natural orbit frequeneies of these eleetrons are not mueh faster (if at all) than vibrational frequeneies. In sueh eases, signifieant breakdown of the BO pieture is to be expeeted. 

If the rotational motion of the molecules is assumed to be entirely unhindered (e.g., by any environment or by collisions with other molecules), it is appropriate to express the time dependence of each of the dipole time correlation functions listed above in terms of a "free rotation" model. For example, when dealing with diatomic molecules, the electronic-vibrational-rotational C(t) appropriate to a specific electronic-vibrational transition becomes ... 

Figure 1.13 Plot of potential energy, V(r), against bond length, r, for the harmonic oscillator model for vibration is the equilibrium bond length. A few energy levels (for v = 0, 1, 2, 3 and 28) and the corresponding wave functions are shown A and B are the classical turning points on the wave function for w = 28...

At low energies, the rotational and vibrational motions of molecules can be considered separately. The simplest model for rotational energy levels is the rigid dumbbell with quantized angular momentum. It has a series of rotational levels having energy... 

The simplest model for vibrational energy levels is the harmonic oscillator, which has allowed levels with energy... 

The assumption of harmonic vibrations and a Gaussian distribution of neighbors is not always valid. Anharmonic vibrations can lead to an incorrect determination of distance, with an apparent mean distance that is shorter than the real value. Measurements should preferably be carried out at low temperatures, and ideally at a range of temperatures, to check for anharmonicity. Model compounds should be measured at the same temperature as the unknown system. It is possible to obtain the real, non-Gaussian, distribution of neighbors from EXAFS, but a model for the distribution is needed and inevitably more parameters are introduced. 

The thirty-two silent modes of Coo have been studied by various techniques [7], the most fruitful being higher-order Raman and infra-red spectroscopy. Because of the molecular nature of solid Cqq, the higher-order spectra are relatively sharp. Thus overtone and combination modes can be resolved, and with the help of a force constant model for the vibrational modes, various observed molecular frequencies can be identified with specific vibrational modes. Using this strategy, the 32 silent intramolecular modes of Ceo have been determined [101, 102]. 

Consider first of all a very simple elassical model for vibrational motion. We have a partiele of mass m attached to a spring, which is anchored to a wall. The particle is initially at rest, with an equilibrium position along the x-axis. If we displace the particle in the +x direction, then experience teaches us that there is a restoring force exerted by the spring. Likewise, if we displace the particle in the —x direction and so compress the spring, then there is also a restoring force. In either case the force acts so as to restore the particle to its rest position Xe-... 

Using a mechanical model and a set of force constants, Popov and Lubuzh (66ZPS498) have calculated vibration frequencies for polyacetylenic groups. But these calculations are rather complex and the data on the IR spectra of acetylenic... 

Models for description of liquids should provide us with an understanding of the dynamic behavior of the molecules, and thus of the routes of chemical reactions in the liquids. While it is often relatively easy to describe the molecular structure and dynamics of the gaseous or the solid state, this is not true for the liquid state. Molecules in liquids can perform vibrations, rotations, and translations. A successful model often used for the description of molecular rotational processes in liquids is the rotational diffusion model, in which it is assumed that the molecules rotate by small angular steps about the molecular rotation axes. One quantity to describe the rotational speed of molecules is the reorientational correlation time T, which is a measure for the average time elapsed when a molecule has rotated through an angle of the order of 1 radian, or approximately 60°. It is indirectly proportional to the velocity of rotational motion. 

Whereas the quasi-chemical theory has been eminently successful in describing the broad outlines, and even some of the details, of the order-disorder phenomenon in metallic solid solutions, several of its assumptions have been shown to be invalid. The manner of its failure, as well as the failure of the average-potential model to describe metallic solutions, indicates that metal atom interactions change radically in going from the pure state to the solution state. It is clear that little further progress may be expected in the formulation of statistical models for metallic solutions until the electronic interactions between solute and solvent species are better understood. In the area of solvent-solute interactions, the elastic model is unfruitful. Better understanding also is needed of the vibrational characteristics of metallic solutions, with respect to the changes in harmonic force constants and those in the anharmonicity of the vibrations. 

The isotope effects of reactions of HD + ions with He, Ne, Ar, and Kr over an energy range from 3 to 20 e.v. are discussed. The results are interpreted in terms of a stripping model for ion-molecule reactions. The technique of wave vector analysis, which has been successful in nuclear stripping reactions, is used. The method is primarily classical, but it incorporates the vibrational and rotational properties of molecule-ions which may be important. Preliminary calculations indicate that this model is relatively insensitive to the vibrational factors of the molecule-ion but depends strongly on rotational parameters. 

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