Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Natural vibrational coordinates

The nature of coordination of anions such as nitrate, perchlorate, and thiocyanate has been studied by both infrared and Raman techniques. In the case of anions, such as nitrate and perchlorate, the vibrational spectra indicate whether they are ionic or coordinated and if coordinated, whether they are unidentate, bidentate or bridging. In the case of thiocyanate, the vibrational spectra are useful in deciding the site of coordination. The change in the site symmetry of the anion upon coordination leads to changes in vibrational spectra of anions like perchlorate, nitrate, perrhenate and hexa-fluorophosphate. These changes in the vibrational spectra have been used to indicate the nature of coordination. [Pg.175]

Fig. 1.10. Description of "natural collision coordinates" for a reaction AB + C — A + BC, s and n. for the collinear case. (Those for the three-dimensional problem are described in ref. [53].) The s is the reaction coordinate, measured from any fixed point O on C to the foot P of the perpendicular from the point P. The n is the vibrational coordinate, i.e., the... Fig. 1.10. Description of "natural collision coordinates" for a reaction AB + C — A + BC, s and n. for the collinear case. (Those for the three-dimensional problem are described in ref. [53].) The s is the reaction coordinate, measured from any fixed point O on C to the foot P of the perpendicular from the point P. The n is the vibrational coordinate, i.e., the...
It is well known from the Bom-Oppenheimer separation [1] that the pattern of energy levels for a typical diatomic molecule consists first of widely separated electronic states (A eiec 20000 cm-1). Each of these states then supports a set of more closely spaced vibrational levels (AEvib 1000 cm-1). Each of these vibrational levels in turn is spanned by closely spaced rotational levels ( A Emt 1 cm-1) and, in the case of open shell molecules, by fine and hyperfine states (A Efs 100 cm-1 and AEhts 0.01 cm-1). The objective is to construct an effective Hamiltonian which is capable of describing the detailed energy levels of the molecule in a single vibrational level of a particular electronic state. It is usual to derive this Hamiltonian in two stages because of the different nature of the electronic and nuclear coordinates. In the first step, which we describe in the present section, we derive a Hamiltonian which acts on all the vibrational states of a single electronic state. The operators thus remain explicitly dependent on the vibrational coordinate R (the intemuclear separation). In the second step, described in section 7.55, we remove the effects of terms in this intermediate Hamiltonian which couple different vibrational levels. The result is an effective Hamiltonian for each vibronic state. [Pg.316]

They proposed a Jahn Teller conical intersection in Fe(CO)5 oi E e nature due to population of the electronic state coupled to e symmetry vibrational coordinates, corresponding to stretching of the equatorial Fe-C and C-0 bonds reached within 21 fs. This is followed by relaxation to the 1 42 state, then again proceeding... [Pg.325]

As written, the CIDs (2.3) and (2.5) apply to Rayleigh scattering. The same expression can be used for Raman optical activity if the property tensors are replaced by corresponding vibrational Raman transition tensors. This enables us to deduce the basic symmetry requirements for natural vibrational ROA 15,5) the same components of aap and G p must span the irreducible representation of the particular normal coordinate of vibration. This can only happen in the chiral point groups C , Dn, O, T, I (which lack improper rotation elements) in which polar and axial tensors of the same rank, such as aaP and G (or e, /SAv6, ) have identical transformation properties. Thus, all the Raman-active vibrations in a chiral molecule should show Raman optical activity. [Pg.156]

Under these condensed-phase conditions it is natural to consider the full A-body potential energy function (ri... rjv) for the material system of interest and to seek to describe the way its details generate the wide variety of collective thermodynamic and kinetic phenomena that have been experimentally observed in condensed matter. For the remainder of this section we suppose that all N particles are the same chemical species and that vectors r, comprise all relevant position, orientation, conformation, and vibration coordinates. For the moment, volume V will be constant. [Pg.37]

As a consequence of the IVR-mediated nature of the multiple-photon excitation process, the vibrational excitation is randomized as the dissociatirai threshold is approached. Hence, the molecule has no memory of the vibrational coordinate that was originally excited. Dissociation therefore occims statistically and can be modelled using the Arrhenius equation or phase-space theories. Mode-selective dissociation is normally not observed. [Pg.26]

It will be assumed that a preliminary vibration analysis of the complete bridge structure has been made, yielding definitions of a series of natural vibration modes i, together with their associated circular frequencies co > and their generalized masses I. Let the dimensionless generalized coordinate associated with mode i be so... [Pg.374]

As in the collinear case, several approaches are possible. Around 1976, three coupled-channel methods had been used in cross-section calculations for 3-PD systems. One of them, developed by Elkowitz and Wyatt [50, 51], used natural collision coordinates (NCC) and local hindered asymmetric-top-vibrator basis sets [41]. Another, developed by Kuppermann and Schatz [106], used asymptotic free rotor and local vibrator basis sets, and different coordinates in different regions of configuration space, similar to those described... [Pg.74]

Thus far we mainly used a two-body point of view. From now on the discussion will emphasize the polyatomic nature of the dynamics of chemical reactions. This is the same transition that is made in books on spectroscopy. These go from boimd AB to boimd ABC, while we go from unbound AB to unbound ABC. There is more than one vibrational coordinate in ABC. Which one is to be imboimd Well, this is very much part of the discussion of Chapter 5. Nor is it only the stretch vibrations that are of interest. The bending vibration of ABC is the carrier of the steric preference during the collision... [Pg.144]

If the anharmonic force field is evaluated at a nonstationary reference geometry in internal coordinates, then the internal coordinate forces can be neglected and the vibrational analysis performed as if based on a stationary reference geometry. This procedure has been widely employed. With the usual choice of internal coordinate systems (e.g., natural internal coordinates) the results obtained in this way for semirigid molecules are as accurate as possible. ... [Pg.19]


See other pages where Natural vibrational coordinates is mentioned: [Pg.1308]    [Pg.26]    [Pg.1308]    [Pg.26]    [Pg.15]    [Pg.46]    [Pg.205]    [Pg.123]    [Pg.125]    [Pg.325]    [Pg.65]    [Pg.242]    [Pg.13]    [Pg.417]    [Pg.119]    [Pg.132]    [Pg.117]    [Pg.353]    [Pg.354]    [Pg.383]    [Pg.386]    [Pg.389]    [Pg.137]    [Pg.145]    [Pg.2343]    [Pg.6342]    [Pg.413]    [Pg.415]    [Pg.422]    [Pg.53]    [Pg.113]    [Pg.335]    [Pg.169]    [Pg.22]    [Pg.18]    [Pg.183]    [Pg.247]    [Pg.77]    [Pg.343]   
See also in sourсe #XX -- [ Pg.26 ]




SEARCH



Coordinates natural

Vibrational coordinate

Vibrational natural

© 2024 chempedia.info