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Arrhenius ?4-factor definition

The analysis, however, shows that, even when all the factors in the denominator of eqn. (46) are Arrhenius factors, reaction rate constants cannot always be determined on their basis. The analysis carried out using graph theory methods shows that it is possible only for definite types of mechanisms, namely for those that correspond to (a) Hamiltonian or (b) strong bi-connected graphs (the latter term is due to Evstigneev) [54]. [Pg.235]

If measurements are carried out over a wide range in l/T there is no reason to expect that either the Arrhenius factor or the activation energy is independent of temperature. Therefore a strict definition of the activation energy... [Pg.74]

We use this knowledge to derive preexponential factors from (2-20) for a few desorption pathways (see Fig. 2.15). The simplest case arises if the partition functions Q and Q in (2-20) are about equal. This corresponds to a transition state that resembles the ground state of the adsorbed molecule. In order to compare (2-20) with the Arrhenius expression (2-15) we need to apply the definition of the activation energy ... [Pg.46]

Marcus and Rice6 made a more detailed analysis of the recombination from the point of view of the reverse reaction, the unimolecular decomposition of ethane, C2Ha - 2CH3. By the principle of microscopic reversibility the transition states must be the same for forward and reverse paths. Although they reached no definite conclusion they pointed out that a very efficient recombination of CH3 radicals would imply a very high Arrhenius A factor for the unimolecular rate constant of the C2H6 decomposition which in turn would be compatible only with a very "loose transition state. Conversely, a very low recombination efficiency would imply a very tight structure for the transition state and a low A factor for the unimolecular decomposition. [Pg.6]

The Prater number (3 - in contrast to eq. (14.25) is related to Ts and not to TG - and the Arrhenius number have a major influence on the development of the T and c profiles. The pore utilization factor qp is therefore dependent upon Arr, (3 and Thiele modulus . The correlation between these four pi-numbers is represented in Fig. 83. For T]p and the following definitions apply ... [Pg.189]

It is quite simple to say that this article deals with Chemical Dynamics. Unfortunately, the simplicity ends here. Indeed, although everybody feels that Chemical Dynamics lies somewhere between Chemical Kinetics and Molecular Dynamics, defining the boundaries between these different fields is generally based more on sur-misal than on knowledge. The main difference between Chemical Kinetics and Chemical Dynamics is that the former is more empirical and the latter essentially mechanical. For this reason, in the present article we do not deal with the details of kinetic theories. These are reviewed excellently elsewhere " The only basic idea which we retain is the reaction rate. Thus the purpose of Chemical Dynamics is to go beyond the definition of the reaction rate of Arrhenius (activation energy and frequency factor) for interpreting it in purely mechanical terms. [Pg.4]

Absolute rate coefficients and Arrhenius parameters have been obtained for the cycloaddition reaction of S( F2,1,0) atoms with a representative series of olefins and acetylenes. The activation energies are small, and they exhibit a trend with molecular structure which is expected for an electro-philic reagent The A-factors show a definite trend which can be attributed to steric repulsions and a generalized secondary a-isotope effect explained by activated complex theory. Secondary a-H/D kinetic isotope effects have been measured and their origin discussed. Hartree-Fock type MO calculations indicate that the primary product of the S( F) + olefin reaction is a ring-distorted, triplet state thi-irane, with a considerable energy barrier with respect to rotation around the C-C bond. [Pg.137]

Theoretical Consideration The decomposition temperature is an important, if not the most important kinetic parameter used in studies of the decomposition processes. It defines the upper limit of reactant stability and the onset of a decomposition reaction. However, temperature is most commonly used only as an additional factor in determination of the Arrhenius parameters. (For instance, Galwey [1] used an average decomposition temperature in his estimations of A values basing on E parameters, known for various substances.) No quantitative definition of the concept of an initial decomposition temperature has been developed, based on a certain specified value of the decomposition rate J, or on parameters related to it (the rate constant k, or the equilibrium pressure of gaseous products Pb)- The detailed interrelation between the decomposition temperature and the molar enthalpy,... [Pg.65]

The two equivalent adiabatic expressions (106.HI) and (124. HI) represent alternatives of the acciarate formulation of the statistical theory of reaction rates, which rest on two other definitions of the activated complex as a virtual state. In general, they do not involve the Arrhenius exponential factor which includes the classical activation energy. [Pg.227]

Our treatment, based on both the collision and the statistical formulations of reaction rate theory, shows that there exist two possibilities for an interpretation of the experimental facts concerning the Arrhenius parameter K for unimolecular reactions. These possibilities correspond to either an adiabatic or a non-adiabatic separation of the overall rotation from the internal molecular motions. The adiabatic separability is accepted in the usual treatment of unimolecular reactions /136/ which rests on transition state theory. To all appearances this assumption is, however, not adequate to the real situation in most unimolecular reactions.The nonadiabatic separation of the reaction coordinate from the overall rotation presents a new, perhaps more reasonable approach to this problem which avoids all unnecessary assumptions concerning the definition of the activated complex and its properties. Thus, for instance, it yields in a simple way the rate equations (7.IV), corresponding to the "normal Arrhenius parameters (6.IV), which are both direct consequences of the general rate equation (2.IV). It also predicts deviations from the normal values of the apparent frequency factor K without any additional assumptions, such that the transition state (AB)" (if there is one) differs more or less from the initial state of the activated molecule (AB). ... [Pg.241]

Once the reactor equations and assumptions have been established, and HDS, HDN, HDA, and HGO reaction rate expressions have been defined, the adsorption coefficient, equilibrium constants, reaction orders, frequency factors, and activation energies can be determined from the experimental data obtained at steady-state conditions by optimization with the Levenberg-Marquardt nonlinear regression algorithm. Using the values of parameters obtained from steady-state experiments, the dynamic TBR model was employed to redetermine the kinetic parameters that were considered as definitive values. The temperature dependencies of all the intrinsic reaction rate constants have been described by the Arrhenius law, which are shown in Table 7.4. [Pg.250]

The input variables are subdivided into controllable variables and parameters. The controllable variables are those quantities whose values can be varied by the experimenter as, for example, initial and boundary conditions of experiments. Empirical and physical constants that are assumed to remain unchanged in a given set or a subset of experiments constitute the parameters of the model. To clarify an ambiguity that may arise from the above definitions let us consider a rate constant that is expressed in the Arrhenius form k = A Qxp — EJRT). In isothermal modeling the rate constant at the assumed temperature, /c, is a parameter. However, if temperature is a controllable variable of the model, then the preexponential factor A and the activation energy are the parameters. [Pg.424]


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See also in sourсe #XX -- [ Pg.66 ]




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