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Shapes of energy surfaces

So far, the preceding considerations have been very useful for characterization of states and for ordering of singlet-state energies relative to (T) with fixed values of K and K. Nevertheless, we could not receive any qualitative ideas about the shapes of energy surfaces as the biradicaloids develop from the normal molecules. For this purpose the introduction of overlap, which we have neglected so far, is necessary. The Hamiltonian matrix for nonorthogonal orbitals A and B for nonsymmetric biradicaloid is... [Pg.62]

In this chapter, we have tried to convince the reader of the usefulness of the dynamical system theory for chemical reactivity studies. Indeed, it is possible to predict which changes may be achieved when internal, external, or methodological parameters are varied from the shape of energy surface or from the topologies of local functions. The structural stability of the gradient vector fields of global and local functions describing chemical systems appears to be an important concept which has to be considered to understand the reactivity. Moreover, the application of the catastrophe theory to chemical reactions enables the description of the mechanisms [27-34,49-52],... [Pg.55]

SHAPES OF ENERGY SURFACES FROM COUPLING COEFFICIENTS... [Pg.110]

Qualitatively the slope, a, changes as ACzg varies, even though the shapes of the parabolas are assumed to be invariant, because the cross-over point has slopes which alter (see Appendix 1, Section A 1.1.3). The Marcus equation, although simple in concept, is remarkably successful, probably because parabolas are good approximations to the shapes of energy surfaces over small regions of space. [Pg.134]

Potential energy surfaces calculated by means of the London equation (5-15) cannot be highly accurate, but the results have been very useful in disclosing the general shape of the surface and the reaction coordinate. The London equation also forms the basis of some semiempirical methods. [Pg.195]

The calculations thus fail to indicate any substantial energy preference for the allowed paths with respect to the forbidden ones. An inspection of the overall shape of the surface confirms, however, that along the allowed CCW path a less steep slope has to be climbed (Fig. 18). The general conclusion is that steric and symmetry factors are so intimately interwoven that it is impossible to distinguish their relative importance in cases where the magnitudes of the two effects are similar. This can perhaps be taken as a warning that orbital symmetry rules should only be applied with some caution to very strained systems. [Pg.21]

The influence of this surface energy can also be clearly seen on the macroscopic shape of liquid droplets, which in the absence of all other forces will always form a shape of minimum surface area - that is, a sphere in a gravity-free system. This is the reason why small mercury droplets are always spherical. [Pg.7]

The solid line in Figure 4 represents a portion of the potential energy surface for a one-step reaction in the gas phase. In condensed phases the surface is lowered by intermolecular attraction. Nonpolar reactions in fluids are often rather insensitive to phase, suggesting that stabilization by attraction is uniform across the surface, lowering it without changing its shape. Repulsions are typically very weak in fluids, but in crystals they can be strong and localized in certain portions of the potential energy surface. Thus repulsions can alter the shape of the surface. [Pg.289]

In the framework of the Born-Oppenheimer approximation, the motion of the nuclei in a molecule being in the zth electronic state characterized by the energy surface E R) and the wavefunction (x, R) is determined by the shape of the surface. After preparation of... [Pg.6]

Prior to minimization, little information is available about the high-dimensional energy surface (3N- 6 dimensions with N atoms). In simple words, the program cannot see the landscape . Ideally, the minimization process should adapt to the shape of the surface and the distance from the minimum. Also, the type of energy minimization procedure used should depend on whether a specific local minimum, or any minimum, is sought. Most programs offer a choice of different optimization methods and the step size may often be chosen interactively. [Pg.42]

DIN EN ISO 8044 defines wear as the progressive loss of material from the surface of a solid body due to mechanical causes, i. e., contact with solid, liquid, or gaseous bodies and relative motion. Wear is manifested in the presence of loosened particles (wear particles) and in the change in material and shape of the surface layer. Thermal, physical, and chemical processes are activated in the case of most wear processes (triboreactions). Wear is fundamentally caused by mechanically transferred energy. [Pg.303]

Rate of Solubility—The rath of solubility of small particles depends on a great number of variables. Eq (12-2) takes into account free surface energy (a) and particle surface (1 /d). These are purely surface considerations, and are scarcely complete in themselves. The shape of the surface and its physical state must also be specified, that is, its relative freedom from contamination which might influence the speed of reaction. The effect of packing density and the extent of agitation imparted to the particles are also important, particularly with regard to exposure of fresh surfaces and formation of possible gas pockets. The liquid and liquid-solid phases jointly are additional important considerations. The volume of the liquid, its temperature, and the amount of dissolved solid already in solution must enter into all calculations. Nor can we ignore the chemical nature of the substances involved in the... [Pg.245]

This function can be plotted on a polar diagram and used to predict the shape of the surface energy plot cusps in the Wulff constmction. The results are semi-quantitative but useful for finding the relative anisotropic surface energy, in that for cubic crystals, minima are found at low-index (111), (110), and (100) orientations. The interested reader is referred to Venables (2000) and Howe (1997) for details. [Pg.80]

Figure 7-2. Potential energy surface by Williams in the region of the transition structure in different representations [21] (a) Three-dimensional representation of the saddle-shaped potential energy surface (b) Two-dimensional potential energy curve produced by a vertical cut through the surface in (a) along the reaction path (indicated by bold dashed line) from reactants (R) to products (P) (c) Energy contours produced by horizontal cuts through the potential energy sufrace in (a). Adapted with permission from Reference [21],... Figure 7-2. Potential energy surface by Williams in the region of the transition structure in different representations [21] (a) Three-dimensional representation of the saddle-shaped potential energy surface (b) Two-dimensional potential energy curve produced by a vertical cut through the surface in (a) along the reaction path (indicated by bold dashed line) from reactants (R) to products (P) (c) Energy contours produced by horizontal cuts through the potential energy sufrace in (a). Adapted with permission from Reference [21],...
Again a negative value for Q indicate.s that net radiation heat transfer is to surface i (i,ej> surface t gains radiation energy instead of losing). Also, the net heat transfer from a surface to itself is zero, regardless of the. shape of the surface. ... [Pg.739]

The surface tension of the system KF-KBF4 decreases with the increasing content of KBF4, obviously due to the covalent character of the bonds in the BFJ complex anions, which are surface active and concentrate on the melt surface. Similar values as well as the shape of the surface adsorption curve were found when it was calculated from the polynomial coefficients and from the excess Gibbs energy of mixing in the liquid phase. Even both the calculated interaction parameters B are relatively close. [Pg.281]


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See also in sourсe #XX -- [ Pg.110 ]




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