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Anharmonic oscillator, energy

Figure 2. Working diagram showing how the linear free-energy relationship, common in electrode process kinetics, arises from changes in electrode potential. is a symmetry factor. An extreme case of an anharmonic oscillator energy profile is shown in schematic form (cf. Ref. 25). This representation assumes changes in V affect only the energy of electrons in the initial state at the Fermi level. Figure 2. Working diagram showing how the linear free-energy relationship, common in electrode process kinetics, arises from changes in electrode potential. is a symmetry factor. An extreme case of an anharmonic oscillator energy profile is shown in schematic form (cf. Ref. 25). This representation assumes changes in V affect only the energy of electrons in the initial state at the Fermi level.
The reason that does not change with isotopic substitution is that it refers to the bond length at the minimum of the potential energy curve (see Figure 1.13), and this curve, whether it refers to the harmonic oscillator approximation (Section 1.3.6) or an anharmonic oscillator (to be discussed in Section 6.1.3.2), does not change with isotopic substitution. Flowever, the vibrational energy levels within the potential energy curve, and therefore tq, are affected by isotopic substitution this is illustrated by the mass-dependence of the vibration frequency demonstrated by Equation (1.68). [Pg.132]

Figure 6.4 Potential energy curve and energy levels for a diatomic molecule behaving as an anharmonic oscillator compared with those for a harmonic oscillator (dashed curve)... Figure 6.4 Potential energy curve and energy levels for a diatomic molecule behaving as an anharmonic oscillator compared with those for a harmonic oscillator (dashed curve)...
To illustrate the anharmonic contribution to RPFR from a particular high frequency mode treated in the ZPE approximation, for example a CH/CD stretch, we recall the oscillator energy neglecting Go is expressed... [Pg.159]

To obtain the allowed energy levels, Ev, for a real diatomic molecule, known as an anharmonic oscillator, one substitutes the potential energy function describing the curve in Fig. 3.2c into the Schrodinger equation the allowed energy levels are... [Pg.44]

When exposed to electromagnetic radiation of the appropriate energy, typically in the infrared, a molecule can interact with the radiation and absorb it, exciting the molecule into the next higher vibrational energy level. For the ideal harmonic oscillator, the selection rules are Av = +1 that is, the vibrational energy can only change by one quantum at a time. However, for anharmonic oscillators, weaker overtone transitions due to Av = +2, + 3, etc. may also be observed because of their nonideal behavior. For polyatomic molecules with more than one fundamental vibration, e.g., as seen in Fig. 3.1a for the water molecule, both overtones and... [Pg.44]

FIGURE 3.2 (a) Vibration of diatomic molecule, HC1, (b) potential energy of an ideal harmonic oscillator, and (c) an anharmonic oscillator described by the Morse function. [Pg.45]

Figure 2. Internuclear separation (top panel) and velocity (bottom panel) as a function of time for a Morse (dashed line) and harmonic (solid line) oscillator having the same total energy, ca. 50% of the dissociation energy of the Morse potential. Note the rapid change in velocity at the inner turning point and slow change in velocity at the outer turning point for an anharmonic oscillator. Figure 2. Internuclear separation (top panel) and velocity (bottom panel) as a function of time for a Morse (dashed line) and harmonic (solid line) oscillator having the same total energy, ca. 50% of the dissociation energy of the Morse potential. Note the rapid change in velocity at the inner turning point and slow change in velocity at the outer turning point for an anharmonic oscillator.
Figure 4. Still shots from movies of the motion of an anharmonic oscillator with a total energy approximately 50% of the dissociation energy. The system starts at the inner turning point and travels to the outer turning point. The students make animations of these plots to compare the observed motion with the calculations plotted in Figures 2. Figure 4. Still shots from movies of the motion of an anharmonic oscillator with a total energy approximately 50% of the dissociation energy. The system starts at the inner turning point and travels to the outer turning point. The students make animations of these plots to compare the observed motion with the calculations plotted in Figures 2.
Energy levels in the anharmonic oscillator are not equal, although they become slightly closer as energy increases. This phenomenon can be seen in the following equation , ... [Pg.373]

S. E. Stein and B. S. Rabinovitch. Accurate Evaluation of Internal Energy Level Sums and Densities Including Anharmonic Oscillators and Hindered Rotors. J. Chem. Phys., 58 2438-2445,1973. [Pg.836]

Theory predicts that for a harmonic oscillator only a change from one vibrational energy level to the next higher is allowed, but for anharmonic oscillators weaker transitions to higher vibrational energy levels can occur. The resulting "overtones" are found at approximate multiples of the frequency of the fundamental. Combination frequencies representing sums... [Pg.1277]

We have shown the molecular orbital theory origin of structure - function relationships for electronic hyperpolarizability. Yet, much of the common language of nonlinear optics is phrased in terms of anharmonic oscillators. How are the molecular orbital and oscillator models reconciled with one another The potential energy function of a spring maps the distortion energy as a function of its displacement. A connection can indeed be drawn between the molecular orbitals of a molecule and its corresponding effective oscillator . [Pg.102]

Anharmonic oscillator-molecular orbital theory connection anharmonic energy profile, 97,98/ two-orbital calculation, 96-97,98/ Anharmonic springs, nonlinear polarizabilities, 90 Anionic group theory assumptions, 364-365... [Pg.720]

In the lowest order of perturbation theory, the energy levels of the three-dimensional anharmonic oscillator are... [Pg.247]

Describe the correlation that may exist between the Morse curve and the energy potential curve of an anharmonic oscillator. [Pg.232]

Rl. Within a molecule, the stretching of the molecular bond lets the atoms come closer and move away one from each other. The Morse curve describes the potential energy induced by this stretching. At short distances, the repulsive forces are dominant, while at long distances, the attractive forces are dominant. However, when the distance that separates the two atoms within the bond is too important, the attractive forces are no longer efficient, and the Morse curve will look like an anharmonic oscillator. [Pg.242]

If there was no interaction between vibration and rotation, the energy levels would be given by the simple sum of the expression giving the vibrational levels for the anharmonic oscillator, equation (6.188), and that describing the rotational levels of the rigid rotor, equation (6.162). There is an interaction, however during a vibration the moment of inertia of the molecule changes, and therefore so also does the rotational constant. We may therefore use a mean value of Bv for the rotational constant of the vibrational level considered, i.e. [Pg.243]

In this case, the zeroth-order Hamiltonian is chosen to represent the vibrational energy of the anharmonic oscillator ... [Pg.338]


See other pages where Anharmonic oscillator, energy is mentioned: [Pg.207]    [Pg.207]    [Pg.144]    [Pg.240]    [Pg.97]    [Pg.82]    [Pg.271]    [Pg.276]    [Pg.311]    [Pg.24]    [Pg.373]    [Pg.133]    [Pg.307]    [Pg.153]    [Pg.260]    [Pg.80]    [Pg.150]    [Pg.108]    [Pg.144]    [Pg.240]    [Pg.11]    [Pg.49]    [Pg.239]    [Pg.634]    [Pg.489]   


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