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Internal modes of vibration

From a molecular viewpoint, we know that heat capacity is closely connected to internal modes of molecular vibration. According to the classical equipartition theorem (Sidebar 3.8), a nonlinear polyatomic molecule of Aat atoms has ftmodes = 3Aat — 6 independent internal modes of vibration, each of which would contribute equally to heat capacity... [Pg.371]

Fig. 6.15 How the six degrees of freedom of free dihydrogen become six internal modes of vibration of an ti -coordinated dihydrogen molecule, (a) Vhh — Vhh. (b) x axis rotation becomes the M-H2 antisymmetric stretch (vHMuasym), (c)y axis rotation becomes the M-H2 torsion, (d) z axis translation becomes the MH2 rock, (e) y axis translation becomes the M-H2 symmetric stretch (vHMusym) and (f) x axis translation becomes the MH2 wag. Fig. 6.15 How the six degrees of freedom of free dihydrogen become six internal modes of vibration of an ti -coordinated dihydrogen molecule, (a) Vhh — Vhh. (b) x axis rotation becomes the M-H2 antisymmetric stretch (vHMuasym), (c)y axis rotation becomes the M-H2 torsion, (d) z axis translation becomes the MH2 rock, (e) y axis translation becomes the M-H2 symmetric stretch (vHMusym) and (f) x axis translation becomes the MH2 wag.
In a two-phonon process which involves an internal mode of vibration for which the frequency p varies little with wave vector, the combined density of states approximates, at least in a cubic crystal, the density of vibrational states spectrum [see Equation (6)]. This is important for a discussion of the absorption that occurs on the high- and low-frequency sides of many internal-mode absorption lines. [Pg.188]

Calculated phonon spectrum for phase I NH3 showing (a) the internal modes of vibration and (b) the external lattice modes of vibration. Note the calculated band intensities are not indicative of the experimental values. Adapted with permission from [10]. Copyright 2008 American Chemical Society. [Pg.247]

Deviations of the absorption pattern from that expected for a free molecule can provide information on the crystal environment. A polyatomic ion containing n atoms has 3n-6 internal modes of vibration and six external modes, corresponding to rotary and translational vibrations of the ion as a whole. Thus, the carbonate and nitrate ions have six internal modes. Owing to the symmetry elements of such ions, one vibration (v. Figure 16) is inactive in the... [Pg.601]

Phonons are nomial modes of vibration of a low-temperatnre solid, where the atomic motions around the equilibrium lattice can be approximated by hannonic vibrations. The coupled atomic vibrations can be diagonalized into uncoupled nonnal modes (phonons) if a hannonic approximation is made. In the simplest analysis of the contribution of phonons to the average internal energy and heat capacity one makes two assumptions (i) the frequency of an elastic wave is independent of the strain amplitude and (ii) the velocities of all elastic waves are equal and independent of the frequency, direction of propagation and the direction of polarization. These two assumptions are used below for all the modes and leads to the famous Debye model. [Pg.412]

Internal thermal noise of mirrors. Mirror substrates are transparent material cylinders. They are affected by thermal noise and each one of their modes of vibration can be represented by an harmonic oscillator. The study of thermal noise in solids is a complex task, made difficult because no... [Pg.322]

Internal conversion refers to radiationless transition between states of the same multiplicity, whereas intersystem crossing refers to such transitions between states of different multiplicities. The difference between the electronic energies is vested as the vibrational energy of the lower state. In the liquid phase, the vibrational energy may be quickly degraded into heat by collision, and in any phase, the differential energy is shared in a polyatomic molecule among various modes of vibration. The theory of radiationless transitions developed by Robinson and Frosch (1963) stresses the Franck-Condon factor. Jortner et al. (1969) have extensively reviewed the situation from the photochemical viewpoint. [Pg.88]

As the oscillators of the OPP model vibrate independently of each other, the frequencies are dispersionless, that is, independent of a wavevector q. For the internal modes of a molecular crystal, this tends to be a very good approximation. For the external modes, the dispersion can be pronounced, as shown in Figs. 2.1 and 2.2. In order to obtain the mean-square vibrational amplitudes for the latter, a summation over all phonon branches in the Brillouin zone must be performed. [Pg.40]

Problem 7-17. Compute the syimnetry species of the normal modes of vibration of CH3 (syimnetry group Dsh) using internal coordinates. [Pg.64]

J.C. Maxwell saw these atoms as capable of internal vibrations 9). Atoms had some form of internal stracture and were not static If there were internal modes of motion in the atoms, Boltzmarm predicted that equipartition of energy would lead to an increased heat capacity. Maxwell worried about the missing heat capacity due to these motions as well. Maxwell died before an explanation of the... [Pg.92]

The complex, random, and seemingly aperiodic internal motions of a vibrating molecule are the result of the superposition of a number of relatively simple vibratory motions known as the normal vibrations or normal modes of vibration of the molecule. Each of these has its own fixed frequency. Naturally, then, when many of them are superposed, the resulting motion must also be periodic, but it may have a period so long as to be difficult to discern. [Pg.305]

The vibrational mode corresponding to altering the separation of the molecules is ca. 0 cm-1 the internal modes of each molecule, bond stretch, bend, and torsional modes, are of course nonzero. [Pg.600]


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See also in sourсe #XX -- [ Pg.538 , Pg.553 , Pg.564 ]




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