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Activation energies barrier height

Cl, C2 Parameters of the WLF equation D Dielectric displacement E Electric field strength Ea Activation energy, barrier heights f Frequency... [Pg.1349]

The height of the energy barrier between the forward and reverse states is the product of the particle volume, V, and the anisotropy constant Kefr (which is, to some extent, a function of particle size). Superparamagnetic relaxation occurs when the thermal energy of the particles exceeds the activation energy barrier between the spin states and so allows rapid, spontaneous fluctuations between these states. The effect of these spin reversals is that the observed magnetic field is reduced or even absent. [Pg.121]

Recall that this equation could be minimized with respect to particle radius to determine the critical particle size, r, as given by Eq. (3.35). This critical radius could then be used to determine the height of the free energy activation energy barrier, AG, as given by Eq. (3.36). A similar derivation can be performed for a cubic particle with edge length, a. [Pg.235]

Figure 4.43 Diffusion in a potential gradient A/x, where AG I is the height of the activation energy barrier and X is the jump distance. From W. D. Kingery, H. K. Bowen, and D. R. Uhlmann, Introduction to Ceramics. Copyright 1976 by John Wiley Sons, Inc. This material is used by permission of John Wiley Sons, Inc. Figure 4.43 Diffusion in a potential gradient A/x, where AG I is the height of the activation energy barrier and X is the jump distance. From W. D. Kingery, H. K. Bowen, and D. R. Uhlmann, Introduction to Ceramics. Copyright 1976 by John Wiley Sons, Inc. This material is used by permission of John Wiley Sons, Inc.
These two examples clearly demonstrate that Ea is not equal to Eq- The temperature dependence of Ea will, however, often be negligible since typically kbT -C Eo-Thus, we have a rough identification of Ea with Eo- It should be remembered that this is not the potential energy barrier height, Ec, but the difference in zero-point energies between the activated complex and the reactants. [Pg.218]

All these reactions are discussed in the framework of a few common potential energy profiles, described in Section I, in which the evolution from the precursor through the intermediate species to the final products is governed by the relative height of the corresponding activation energy barriers. [Pg.67]

The actual path followed will clearly depend on the heights of the activation energy barriers for the individual steps, so that the overall rate is maximized. In general, only one pathway, and rate-determining step, will predominate on a given surface. There may be occasional exceptions to this rule, particularly in the case of the reduction of molecular oxygen. These are discussed in a later section. [Pg.180]

Values of barrier heights vary widely between chemical reactions. They control how rapidly reactions take place and how their rates respond to changes in temperature. (Most reactions involve a number of steps and the activation energy may not correspond to the height of any individual activation energy barrier. It is a concept best applied to the individual elementary steps of a multi-step reaction.)... [Pg.200]

The kinetics of deposition can be modeled as an activated process, and the rate of deposition will depend on the energy barrier height, A F. To examine the functional dependence of A on various experimental parameters, we consider that the interaction potential between the charged DNA-SWCNTs and the substrate consists of two components, electrostatic repulsion and van der Waals attraction, as in DLVO theory. The interaction potential depends on separation between, and relative orientation of, the DNA-SWCNT and the surface. The potential barrier is lowest when the axis of the DNA-SWCNT is perpendicular to the surface. This has been confirmed numerically we have previously examined deposition by thermal hopping over an electrostatic energy barrier of DNA-SWCNT rods aligned parallel to the substrate" in order to explain a different set of experiments, and the potential barrier can be far higher. [Pg.632]

Fig. 9.22 A proton can tunnel through the activation energy barrier that separates reactants from products, so the effective height of the barrier is reduced and the rate of the proton transfer reaction increases. The effect is represented by drawing the wavefunction of the proton near the barrier. Proton tunneling is important only at low temperatures, when most of the reactants are trapped on the left of the barrier. Fig. 9.22 A proton can tunnel through the activation energy barrier that separates reactants from products, so the effective height of the barrier is reduced and the rate of the proton transfer reaction increases. The effect is represented by drawing the wavefunction of the proton near the barrier. Proton tunneling is important only at low temperatures, when most of the reactants are trapped on the left of the barrier.

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See also in sourсe #XX -- [ Pg.88 ]




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