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Interatomic equilibrium distance

The vibrational and rotational constants are now written as a>c and Be. They may be thought of as the values that correspond to the equilibrium interatomic distance of minimum potential energy.J The first and third terms are expressions... [Pg.558]

The van der Waals forces are present universally, regardless of the species and polarity of the interacting atoms or molecules. The forces can be attractive or repulsive, but mostly attractive and long-range, effective from a distance longer than 10 nm down to the equilibrium interatomic distance (about 0.2 nm). [Pg.168]

The multiplicity of symmetry breakings have been explored in details in N2 where they occur near the equilibrium interatomic distance [12]. [Pg.106]

Table 2. Heats offormation, H (kcal), magnitude of electron density, Q (Of), displace from the cluster to adsorbed oxygen molecules, equilibrium interatomic distances R (A-B) and bond orders P (A-B), corresponding to them, in PANI-O2 adsorption complexes. Table 2. Heats offormation, H (kcal), magnitude of electron density, Q (Of), displace from the cluster to adsorbed oxygen molecules, equilibrium interatomic distances R (A-B) and bond orders P (A-B), corresponding to them, in PANI-O2 adsorption complexes.
The Band Theory of Crystalline Solids. Consider a crystalline solid. The atoms are arranged according to a three-dimensional pattern (or lattice) in which they have equilibrium interatomic distances. A thought experiment is now performed. The lattice is expanded, i.e., the interatomic distances are increased. [Pg.268]

This means that as the expanded lattice is contracted in the thought experiment, the discrete energy states of the atoms are replaced by energy bands. Thus, when the lattice-contraction thought experiment is finally halted with atoms at their equilibrium interatomic distances, the electron-energy states show a band structure. [Pg.269]

The energy states of gaseous atoms split because of the overlap between electron clouds. Obviously, therefore, atoms must come much closer before the clouds of the core electrons begin to overlap compared with the distance at which the clouds of outer (or valence) electrons overlap (Fig. 6.119). Hence, at the equilibrium interatomic distances, the energy levels of the core electrons (in contrast to the valence electrons) do not show any band structure and therefore will be neglected in the following discussion. This simplified picture of the band theory of solids will now be used to explain the differences in conductivity of metals, semiconductors, and insulators. [Pg.270]

For all the polyacenes studied the first maximum in the kinetic spectrum always exceeds the work function by 0.8 e.v. This excess can be explained by the vertical Franck-Condon transition from the potential surface of the neutral molecule to that of the positive molecular ion, which possess different equilibrium interatomic distances. [Pg.417]

The numerical value of the coefficient C2 is -0.20734 for the equilibrium interatomic distance in methane. The above form of the HO transformation matrix is perfectly confirmed by our numerical experiments performed within the FA picture even for very large distortions, which is a consequence of the mathematical structure of the hybridization manifold described above. The numerical data show that the linear response estimate performs very well up to improbably large distortions (the deviation from the linear response estimate is smaller than 0.25% for the distortion of 0.3 rad (about 17°)). [Pg.256]

In order to test the point-charge method experimentally measured dissociation energy and interatomic distance are required for each chemical bond. Dissociation energies for most homonuclear diatomic molecules have been measured spectroscopically and/or thermochemically. Interatomic distances for a large number of these are also known. However, for a large number of, especially metallic diatomic molecules, equilibrium interatomic distances have not been measured spectroscopically. In order to include these elements in the sample it is noted that for those metals with measured re, it is found to be related, on average, to 5, the distance of closest approach in the metal, by re = 0.78(5. On this assumption reference values of interatomic distance (d) become available for virtually all elements, as shown in the data appendix. In some special cases well-characterized dimetal bond lengths have also been taken into account for final assessment of interatomic distance. [Pg.175]

This equation gives the lattice energy in joules per mole. We can avoid having to determine a value for the parameter B by using the equilibrium interatomic distance as the value of r for which U is a minimum. This gives dU /dr = 0... [Pg.67]

The empirical mPBE functional39 discussed in the previous section leads to slightly better equilibrium interatomic distances for the He2, Ne2, and Ar2 dimers without, however, affecting the interaction energies compared to the parent functional (PBE). [Pg.179]

Fig. 4 Map of the validity regimes of the several contact mechanics models (adhesion map). Pad/P denotes the ratio between the adhesive component of the load and the total one. Si is the elastic compression, whereas Sad is the deformation due to adhesion. h0 is the effective range of action of adhesive forces (h0=Q.97z0, whereby z0 denotes the equilibrium interatomic distance). Adapted from [108]... Fig. 4 Map of the validity regimes of the several contact mechanics models (adhesion map). Pad/P denotes the ratio between the adhesive component of the load and the total one. Si is the elastic compression, whereas Sad is the deformation due to adhesion. h0 is the effective range of action of adhesive forces (h0=Q.97z0, whereby z0 denotes the equilibrium interatomic distance). Adapted from [108]...
Two of its three adjustable parameters, De and re correspond to directly measurable molecular properties of bond dissociation energy and equilibrium interatomic distance respectively. The third parameter, a, is related to the force constants commonly used in spectroscopic analyses. A standard procedure [147] to obtain experimental potential energy curves is to calculate from spectroscopic data the constants ke, g, and j that appear in the expression... [Pg.161]

The equilibrium interatomic distance Rq is assumed to be known, in addition to the compressibility k and the molar volume Tq. Actually, only a limited number of reliable values for k are known, but regularities in Vq/k allow reasonable estimates to be made in other cases. When Z is 2 or 3 small errors in these estimates can lead to large errors in the equilibrium potential energy Uq. [Pg.130]

For crystalline solids, the equilibrium interatomic distance, r0, can be estimated from knowledge of lattice site separation distances and is typically expressed as some fraction of the lattice parameter ac. Aluminum forms a face-centered-cubic (fee) lattice, with lattice parameter ac = 0.405 nm. Since the densest packing direction is along the face diagonal, i.e., along the (110) direction, the equilibrium interatomic distance in Al is 4la /2 = 0 29nm. We can also calculate the distance... [Pg.14]

Fig. 5.16. Schematic representation of the spreading of the 3s and 3p energy levels of isolated sodium atoms as the atoms condense to form a crystal. The broken line represents the equilibrium interatomic distance in the solid. Fig. 5.16. Schematic representation of the spreading of the 3s and 3p energy levels of isolated sodium atoms as the atoms condense to form a crystal. The broken line represents the equilibrium interatomic distance in the solid.
Ionic bonds are formed by the transfer of electrons from an electropositive to an electronegative atom. The long-range coulombic attraction of these charged species for each other, together with a short-range repulsive energy component, results in the formation of an ionic bond at an equilibrium interatomic distance. [Pg.47]

Show that Eqs. (11.2) and (11.9) are equivalent, provided the radius of curvature of the crack p w 14ro, where tq is the equilibrium interatomic distance in other words, if it is assumed that the crack is atomically sharp. Hint Find expressions for 7 and Y in terms of m, and r defined in Chap. 4. You can assume n — 9 and m—. ... [Pg.395]

Since no precise physical significance can be attached to the concept of atomic or ionic radius (the electronic wave functions approach zero asymptotically), the radii to be assigned are those which reproduce the equilibrium interatomic distances in ionic crystals. These distances depend on the balance between the attractive and repulsive forces, and thus not only on the electron distributions of the ions but also on the crystal structure and the radius ratios. Pauling assumes that the relative sizes of a pair of isoelec-tronic ions are inversely proportional to the effective nuclear charges operating on the outmost electron shell that is... [Pg.54]

At equilibrium dV/dR = 0 and R2 = (nB/Az2y,(-n 1). If the ions were to enter into Coulomb attraction as if they were monovalent, with the repulsion coefficient unchanged, the equilibrium interatomic distance would be... [Pg.55]

Fig. 4.4. Atomic level splitting into energy bands to form a metallic bond. The equilibrium interatomic distance is ro. Fig. 4.4. Atomic level splitting into energy bands to form a metallic bond. The equilibrium interatomic distance is ro.

See other pages where Interatomic equilibrium distance is mentioned: [Pg.297]    [Pg.372]    [Pg.108]    [Pg.309]    [Pg.332]    [Pg.158]    [Pg.178]    [Pg.193]    [Pg.308]    [Pg.2407]    [Pg.105]    [Pg.149]    [Pg.423]    [Pg.313]    [Pg.330]    [Pg.71]    [Pg.529]    [Pg.268]    [Pg.149]    [Pg.103]    [Pg.362]    [Pg.498]    [Pg.2406]    [Pg.372]    [Pg.5]   
See also in sourсe #XX -- [ Pg.69 , Pg.70 , Pg.175 , Pg.193 ]

See also in sourсe #XX -- [ Pg.161 ]




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Interatomic

Interatomic distances

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