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Equilibrium bond distance

Most of the molecules we shall be interested in are polyatomic. In polyatomic molecules, each atom is held in place by one or more chemical bonds. Each chemical bond may be modeled as a harmonic oscillator in a space defined by its potential energy as a function of the degree of stretching or compression of the bond along its axis (Fig. 4-3). The potential energy function V = kx j2 from Eq. (4-8), or W = ki/2) ri — riof in temis of internal coordinates, is a parabola open upward in the V vs. r plane, where r replaces x as the extension of the rth chemical bond. The force constant ki and the equilibrium bond distance riQ, unique to each chemical bond, are typical force field parameters. Because there are many bonds, the potential energy-bond axis space is a many-dimensional space. [Pg.97]

There is very little experimental data available for H2", apart from the dissociation energy and equilibrium bond distance. [Pg.76]

Table 1 Calculated equilibrium bond distances [A] of the dihalogens as obtained with different methods applying the aug-cc-pVTZ basis set [35]... Table 1 Calculated equilibrium bond distances [A] of the dihalogens as obtained with different methods applying the aug-cc-pVTZ basis set [35]...
The C=C harmonic vibrational frequency is calculated at 1671 cm-1 in free ethylene and is infrared (IR) forbidden. Its IR intensity is therefore expected to remain low in the vinyl series of compounds. The C=C stretch energy is calculated to be 1687 cm-1 in propene and then decline to 1629 4 cm-1 for X = Si - Pb. As in the equilibrium bond distance, there is also a very small counter-trend change in the vibrational frequency going from X = Sn to X = Pb that indicates a slight strengthening of the C=C bond. [Pg.61]

We are interested in more complex molecules such as [Fe(H20)e]2+-As we discussed in Chapter 6, the equilibrium bond distance between... [Pg.260]

Figure 2.3 A Morse curve for a diatomic molecule, showing the quantised vibrational energy levels. The minimum on the curve represents the equilibrium bond distance, re... Figure 2.3 A Morse curve for a diatomic molecule, showing the quantised vibrational energy levels. The minimum on the curve represents the equilibrium bond distance, re...
Fig. 9. Correlation potential Vff and its components for H2 at the equilibrium bond distance of 1.4 a.u. Potentials are plotted along the bond axis as functions of the distance R from the bond midpoint. The H nucleus is at R = 0.7 a.u. Fig. 9. Correlation potential Vff and its components for H2 at the equilibrium bond distance of 1.4 a.u. Potentials are plotted along the bond axis as functions of the distance R from the bond midpoint. The H nucleus is at R = 0.7 a.u.
Equilibrium Bond Distance and the Harmonic Frequency for N2 from the 2-RDM Method with 2-Positivity (DQG) Conditions Compared with Their Values from Coupled-Cluster Singles-Doubles with Perturbative Triples (CCD(T)), Multireference Second-Order Perturbation Theory (MRPT), Multireference Configuration Interaction with Single-Double Excitations (MRCI), and Full Configuration Interaction (FCI)". [Pg.50]

We have employed the nongradient geometry optimization to determine the equilibrium bond distances (r ). For each molecule, we have calculated the total energy U r) at a dense grid of bond distances r, separated from each other by 10 A. The harmonic vibrational frequencies (cOe) were determined from the second derivatives of the energy with respect to the nuclear positions. The... [Pg.421]

The performance of our practical NOF to predict equilibrium bond distances and vibrational frequencies is similar to CCD. [Pg.423]

A goal of this chapter is to show, for the diatomic molecules under discussion, both the capability of the VB method in providing quantitative estimates of molecular properties and its capability of giving qualitative pictures of the bonding. The quantitative results are illustrated in Table 11.1, where we give values for Rg, the equilibrium bond distance, and determined theoretically with ST03G, 6-3IG,... [Pg.146]

Table 13.5. Principal standard tableaux function structures for CH at equilibrium bond distances. Table 13.5. Principal standard tableaux function structures for CH at equilibrium bond distances.
The most conspicuous difference between the data presented in Table 9-1 and previous comparisons involving equilibrium bond distances (see Chapter 5) are the much larger variations among different models. This should not come as a surprise. Transition states represent a compromise situation where some bonds are being broken while others are being formed, and the potential energy surface around the transition state would be expected to be flat. ... [Pg.295]

We will see later on that we can use this expression to convert between force and energy for specific types of atoms and molecules (specific values of n and m). For now, this expression helps us find the equilibrium bond distance, ro, which occurs when forces are equal (the sum of attractive and repulsive forces is zero) or at minimum potential energy (take the derivative and set it equal to zero) ... [Pg.14]

Work with a neighbor. Consider the Lennard-Jones potential, as given by Eq. (1.12), for which m = 6 and w = 12. Yon wish to determine the separation distance, r, at which the maximum force occurs, in terms of the equilibrium bond distance, ro. [Pg.16]

Person 1 Use Eq. (1.16) with the values of m and n of the Lennard-Jones potential to solve for the constant a in terms of b and the equilibrium bond distance, ro. Now perform the determination of F ax as given by Eq. (1.15) substitute this value of a back into Eq. (1.12), differentiate it twice with respect to r (remember that ro is a constant), and set this equal to zero (determine, then maximize the force function). Solve this equation for r in terms of tq. The other constant should drop out. [Pg.16]


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