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Eneigy barrier height

Energy Barrier. An eneigy barrier results in repulsive forces between droplets when they approach each other. The half-life of an emulsion changes drastically when eneigy barriers of different height are introduced in the system. Increasing the barrier to 20 kT gives a typical half-life of a few years which is sufficient for most applications. [Pg.199]

Fig. 14A The reaction H2 + OH H2O + H eneigy profile V )(s) for —00 < s < 00. The value of the reaction coordinate i = —00 corresponds to the reactants, while = 00 correspraids to the products. It turns out that the product energy (shown by a small square on the right) is lower than the energy of the reactants (i.e., the reaction is exothermic). The barrier height in the entrance channel calculated as the difference of the top of the barrier and the lowest point of the entrance channel amounts to 6.2 kcal/mol. Source T. Dunning, Jr. and E. Kraka. from At/wo/rccs in Molecular Electronic Structure Theory, ed. T. Dunning, Jr., JAI Press, Greenwich, CT (1989), courtesy of the authors. Fig. 14A The reaction H2 + OH H2O + H eneigy profile V )(s) for —00 < s < 00. The value of the reaction coordinate i = —00 corresponds to the reactants, while = 00 correspraids to the products. It turns out that the product energy (shown by a small square on the right) is lower than the energy of the reactants (i.e., the reaction is exothermic). The barrier height in the entrance channel calculated as the difference of the top of the barrier and the lowest point of the entrance channel amounts to 6.2 kcal/mol. Source T. Dunning, Jr. and E. Kraka. from At/wo/rccs in Molecular Electronic Structure Theory, ed. T. Dunning, Jr., JAI Press, Greenwich, CT (1989), courtesy of the authors.
Schaefer [26] has reviewed many of the calculations for this system. Extensive Cl with large basis sets yielded a theoretical barrier height of 13.6 kJ mol l which is considerably laiger than the experimental activation eneigy which is of the order of... [Pg.386]

Fig. 4.2 Schematic illustration of the threshold resonances (a) and queintum dynamical resonance (b), adapted from [67]. In each panel, the left figure illustrates the effective dynamical potential along the reaction coordinate R, and the middle and the right ones tire the c-dependence of the reaction probability Pj Ef) and the reaction cross section a(Ec). In the case of threshold resonance, the non-zero values of the reaction probability and cross section start at a smaller collision energy than the height of the barrier, which manifests the effect of zero-point eneigy... Fig. 4.2 Schematic illustration of the threshold resonances (a) and queintum dynamical resonance (b), adapted from [67]. In each panel, the left figure illustrates the effective dynamical potential along the reaction coordinate R, and the middle and the right ones tire the c-dependence of the reaction probability Pj Ef) and the reaction cross section a(Ec). In the case of threshold resonance, the non-zero values of the reaction probability and cross section start at a smaller collision energy than the height of the barrier, which manifests the effect of zero-point eneigy...
Figure 2.5 depicts a simple example. A particle with eneigy E collides with a rectangular potential barrier of height C/b > E. In classical mechanics it will be simply reflected back. In reality there is a finite probability that it will tunnel to the... [Pg.101]


See other pages where Eneigy barrier height is mentioned: [Pg.245]    [Pg.737]    [Pg.199]    [Pg.374]    [Pg.199]    [Pg.911]    [Pg.948]    [Pg.130]    [Pg.54]    [Pg.601]    [Pg.161]    [Pg.443]    [Pg.181]    [Pg.2041]    [Pg.590]   
See also in sourсe #XX -- [ Pg.220 ]




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