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Anharmonic correction

2 Anharmonicity Internal Modes, Effect of Zero Point Anharmonicity [Pg.158]

In Equation 5.34 to is the harmonic frequency, v the vibrational quantum number, and xe and ye the first and second anharmonicity constants (mass dependent, co x /(coxe) = X /X = il/il, l, and i are vibrational reduced masses). The ZPE(v = 0) contribution to RPFR through first order is thus [Pg.159]

The best fit harmonic approximation, on the other hand, gives [Pg.159]

5 Condensed Phase Isotope Effects Isotope Effects in Non-ideal Gases [Pg.160]

The most important part of the anharmonic correction to isotope exchange equilibria is in the zero point energy term. [Pg.15]

The full theory of this correction was developed by Wolfsberg in 1967 (35). We shall outline here the theory for a diatomic molecule [Pg.15]

ACS Symposium Series American Chemical Society Washington, DC, 1975. [Pg.15]

s (19 - 23), Q Is the normal coordinate and the other terms have the usual spectroscopic significance. The Important new term introduced by Wolfsberg is Gq. This correction may be as large as the 1/4 x U) correction in Eq. (20) and may be of the same or opposite ii n. Wolfsberg has extended this method to the water and ammonia molecules. In Fig. II we reproduce the comparison of Bron and Wolfsberg s (36) calculation of exchange equilibrium [Pg.16]


The LIN method ( Langevin/Implicit/Normal-Modes ) combines frequent solutions of the linearized equations of motions with anharmonic corrections implemented by implicit integration at a large timestep. Namely, we express the collective position vector of the system as X t) = Xh t) + Z t). (In LN, Z t) is zero). The first part of LIN solves the linearized Langevin equation for the harmonic reference component of the motion, Xh t)- The second part computes the residual component, Z(t), with a large timestep. [Pg.246]

It is possible to use computational techniques to gain insight into the vibrational motion of molecules. There are a number of computational methods available that have varying degrees of accuracy. These methods can be powerful tools if the user is aware of their strengths and weaknesses. The user is advised to use ah initio or DFT calculations with an appropriate scale factor if at all possible. Anharmonic corrections should be considered only if very-high-accuracy results are necessary. Semiempirical and molecular mechanics methods should be tried cautiously when the molecular system prevents using the other methods mentioned. [Pg.96]

An anharmonic correction for the density of states was also evaluated by solving the phase integral for the Cl-—CH3C1 intermolecular complex 39 i.e. ... [Pg.149]

Fig. 7. Predicted diffusion coefficients for hydrogen (H) and deuterium (D) in niobium, as calculated by Schober and Stoneham (1988) from a model taking account of tunneling between various states of vibrational excitation and comparison with experimental measurements (solid lines). Theoretical curves are shown both for a model using harmonic vibrational wave functions (dashed lines) and for a model with anharmonic corrections (dashed-dotted lines). Fig. 7. Predicted diffusion coefficients for hydrogen (H) and deuterium (D) in niobium, as calculated by Schober and Stoneham (1988) from a model taking account of tunneling between various states of vibrational excitation and comparison with experimental measurements (solid lines). Theoretical curves are shown both for a model using harmonic vibrational wave functions (dashed lines) and for a model with anharmonic corrections (dashed-dotted lines).
A method for determining anharmonicity corrections to C. K. force field is proposed... [Pg.149]

Although the harmonic ZPVE must always be taken into account in the calculation of AEs, the anharmonic contribution is much smaller (but oppositely directed) and may sometimes be neglected. However, for molecules such as H2O, NH3, and CH4, the anharmonic corrections to the AEs amount to 0.9, 1.5, and 2.3 kJ/mol and thus cannot be neglected in high-precision calculations of thermochemical data. Comparing the harmonic and anharmonic contributions, it is clear that a treatment that goes beyond second order in perturbation theory is not necessary as it would give contributions that are small compared with the errors in the electronic-structure calculations. [Pg.23]

The terms with K and k are anharmonic corrections that can still be dealt with analytically in the algebraic approach. An alternative form of Eq. (2.104) can be obtained by introducing the operators of Table 2.1. In terms of these operators... [Pg.43]

It is instructive to calculate the anharmonic correction to the zero point energy contribution to fractionation factors for isotope exchange equilibria involving hydrogen and deuterium. For example consider the exchange... [Pg.135]

Isotope effects on anharmonic corrections to ZPE drop off rapidly with mass and are usually neglected. The ideas presented above obviously carry over to exchange equilibria involving polyatomic molecules. Unfortunately, however, there are very few polyatomics on which spectroscopic vibrational analysis has been carried in enough detail to furnish spectroscopic values for Go and o)exe. For that reason anharmonic corrections to ZPE s of polyatomics have been generally ignored, but see Section 5.6.3.2 for a discussion of an exception also theoretical (quantum package) calculations of anharmonic constants are now practical (see above), and in the future one can expect more attention to anharmonic corrections of ZPE s. [Pg.136]

We shall not present all terms for perturbation corrections from the right hand side of eq. (85). There are corrections which corresponds to electron correlation, anharmonicity corrections and adiabatic corrections [25]. We shall pay attention only to adiabatic... [Pg.397]

However, the very low values currently reported (P) depend in turn on the procedure used (44) for estimating anharmonicity corrections. [Pg.6]

Wu and Farges (1999) have made use of eqn (9.17) relating bond valence to the coefficient of thermal expansion to confirm that it is possible to resolve the different thermal expansions of the long and short Th-O bonds in thorite (o -ThSi04) from XAFS spectra measured between room temperature and 1700K. They also use this relation to estimate the anharmonic corrections needed for the bond lengths determined from XAFS (Brown et al. 1995, pp. 358-9). [Pg.194]

Fig. 6.4 Vibrational energy levels of a molecule with >, 3800 cm-1, v2wk 1600 cm-1, and p3 3900 cm-1. (These are roughly the values for H20.) The energy is calculated from (6.54), and does not include anharmonicity corrections. Fig. 6.4 Vibrational energy levels of a molecule with >, 3800 cm-1, v2wk 1600 cm-1, and p3 3900 cm-1. (These are roughly the values for H20.) The energy is calculated from (6.54), and does not include anharmonicity corrections.
The formula (6.56), which includes anharmonicity corrections, is applicable only to molecules with no degenerate vibrational modes. Degenerate... [Pg.142]


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See also in sourсe #XX -- [ Pg.134 , Pg.157 , Pg.158 , Pg.159 ]

See also in sourсe #XX -- [ Pg.207 ]

See also in sourсe #XX -- [ Pg.167 ]




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