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Reversible activation energies

This is the general expression for film growth under an electric field. The same basic relationship can be derived if the forward and reverse rate constants, k, are regarded as different, and the forward and reverse activation energies, AG are correspondingly different these parameters are equilibrium parameters, and are both incorporated into the constant A. The parameters A and B are constants for a particular oxide A has units of current density (Am" ) and B has units of reciprocal electric field (mV ). Equation 1.114 has two limiting approximations. [Pg.130]

Fig. 2.14. Influence of the reverse activation energy on KER and thus, on peak shapes in metastable ion decompositions, suitable experimental setup as prerequisite. From left no or small reverse barrier causes Gaussian peak shape, whereas medium or yields flat-topped peaks and large For causes dish-shaped peaks. Fig. 2.14. Influence of the reverse activation energy on KER and thus, on peak shapes in metastable ion decompositions, suitable experimental setup as prerequisite. From left no or small reverse barrier causes Gaussian peak shape, whereas medium or yields flat-topped peaks and large For causes dish-shaped peaks.
The techniques used for the determination of appearance energies are essentially identical to those described above for lEs. However, even when using the most accurately defined electron or photon energies, great care has to be taken when AEs are to be determined because of the risk of overestimation due to kinetic shift. Provided that there is no reverse activation energy for the reaction under study, the AE value also delivers the sum of heats of formation of the dissociation products. If substantial KER is observed, the AE may still be used to determine the activation energy of the process. [Pg.48]

Hvistendahl, G. Williams, D.H. Partitioning of Reverse Activation Energy Between Kinetic and Internal Energy in Reactions of Organic Ions. J. Chem. Soc., Perkin Trans. 2 1975, 881-885. [Pg.62]

Note The validity of Stevenson s rule requires no reverse activation energy barrier to exist for the fragmentation pathway. This requirement is usually fulfilled for simple bond cleavages, but not in case of rearrangement fragmentations. [Pg.232]

Whereas A17 is a thermodynamic quantity that can be obtained from calorimetric measurements, E f and E must be found from the temperature dependence of the rate constants for the forward and reverse reactions. In this reaction the forward and reverse activation energies are 132 and 358 kj moP, respectively, and AU from thermodynamics is 226 kJ moP. ... [Pg.772]

Discuss the connection between activation energy and the energy distribntion of molecules, and relate the forward and reverse activation energies to each other through thermodynamics (Section 18.5, Problems 41-42). [Pg.784]

For the reverse reaction to occur, some molecules on the right (AB) must have kinetic energy equal to the reverse activation energy, E reverse allow them to reach the transition state. As you can see from the potential energy diagrams in Figure 16-10,... [Pg.679]

Relating the heat of reaction to the forward and reverse activation energies (521) ... [Pg.534]

This section is divided into reactions that are treated in terms of vibrator transition states and those that are treated with flexible, or rotator type transition states. Reactions with reverse activation energies have saddle points in the potential energy surface [fig. [Pg.215]

Vibrator TS for Reactions with No Reverse Activation Energies... [Pg.220]

Analytic potential energy functions for unimolecular reactions without reverse activation energies can be obtained by semi-empirical methods or by ab initio calculations, and enhanced by experimental information such as vibrational frequencies, bond energies, etc. To determine microcanonical VTST rate constants from such a potential function, the minimum in the sum of states along the reaction path must be determined. Two approaches have been used to calculate this sum of states. [Pg.244]

The statistical dissociation rate constant can be calculated from the point of view of the reverse reaction, namely the recombination of the products to form a complex. This approach, commonly referred to as phase space theory (PST) (Pechukas and Light, 1965 Pechukas et al., 1966 Nikitin, 1965 Klots, 1971, 1972) is limited to reactions with no reverse activation energy, that is, reactions with very loose transition states. PST assumes the decomposition of a molecule or collision complex is governed by the phase space available to each product under strict conservation of energy and angular momentum. The loose transition state limit assumes that the reaction potential energy surface is of no importance in determining the unimolecular rate constant. [Pg.254]

The kinetic energy release for the loss of OH from the 2-nitrotoluene ion has been reported . The relatively small value, 20-50 meV , is characteristic of reactions involving a simple bond cleavage with neglectable reverse activation energy. This implies that the final step, in a by-necessity complex reaction, is likely to be a simple bond cleavage. [Pg.264]

This equation relates the enthalpy of the reaction, which is a thermodynamic property, with the direct (E) and reverse ( ) activation energies. If the reaction is exothermic, the enthalpy AH < 0 and, therefore, E < E. Therefore, the direct activation energy is always lower than the reverse, and, consequently, the direct reaction is facilitated because the lower the activation energy, the easier the reaction occurs. The opposite happens with endothermic reactions, in which the enthalpy AH > 0, and, therefore E < E. In this context, the reverse reaction is easier. [Pg.47]

Note that the direct (rj) and reverse (tr) rate increase with the increase in temperature and are always positive. Moreover, the direct and reverse activation energies are always positive. Therefore, the variation of the rate with the increase in temperature is always positive. However, depending on whether the reaction is exothermic (AH < 0 and < E ), the variation of the resulting rate will depend on the difference Evi-ETf Therefore, the resulting rate increases and is always positive, and when the reverse rate increases, the resulting rate reaches a maximum value and decreases positively (according to Figure 3.5). Thus ... [Pg.47]


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See also in sourсe #XX -- [ Pg.212 ]




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