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Two-body rate constant

Figure 2 Dependence on C2H4 density of the effective two-body rate constant of thermal electron attachment in O2-C2H4 mixtures at room temperature. (From Ref. 52.) The dashed curve represents the expected contribution from the BB mechanism. Figure 2 Dependence on C2H4 density of the effective two-body rate constant of thermal electron attachment in O2-C2H4 mixtures at room temperature. (From Ref. 52.) The dashed curve represents the expected contribution from the BB mechanism.
In terms of the above discussion the intercept in Figure 4 corresponds to a limiting (infinite pressure) two body rate constant, ku of 4 X 10"12 cm.3 sec."1. This value is considerably lower than the minimum values for ki which can be estimated from several other studies [2.5 X 10"11 (13), 4 X 10"11 (5), 7 X 10"11 (8,10)]. Because of this inconsistency the value of ki determined from the present results should be considered to be in doubt. Experiments are presently being carried out to clarify this point. [Pg.231]

Figure 4. Dependence of the product of the electron half-life and the oxygen pressure (proportional to the reciprocal of the effective two body rate constant, see text) on the reciprocal air... Figure 4. Dependence of the product of the electron half-life and the oxygen pressure (proportional to the reciprocal of the effective two body rate constant, see text) on the reciprocal air...
X lo cm molecule s has been reached where three-body recombination by M and quenching by M is balanced. From the slope of the plot of Icm vs. total pressure a three-body rate constant of 7 x 10 cm molecule s was determined. As a consequence, the air glowreaction proceeds by a two-body as well as by a three-body reaction. When the air glow rate constant is compared with the total recombination rate of NO + O + M, which also was measured in the chamber, it can be concluded that the air glow rate constant represents within the error limits the total recombination rate constant. Further details are given in the publications Becker et al. (1972c) and (1973). [Pg.16]

Two-body rate amstauti Three-body rate constant ... [Pg.131]

This is connnonly known as the transition state theory approximation to the rate constant. Note that all one needs to do to evaluate (A3.11.187) is to detennine the partition function of the reagents and transition state, which is a problem in statistical mechanics rather than dynamics. This makes transition state theory a very usefiil approach for many applications. However, what is left out are two potentially important effects, tiiimelling and barrier recrossing, bodi of which lead to CRTs that differ from the sum of step frmctions assumed in (A3.11.1831. [Pg.993]

This review focuses on the kinetics of reactions of the silicon, germanium, and tin hydrides with radicals. In the past two decades, progress in determining the absolute kinetics of radical reactions in general has been rapid. The quantitation of kinetics of radical reactions involving the Group 14 metal hydrides in condensed phase has been particularly noteworthy, progressing from a few absolute rate constants available before 1980 to a considerable body of data we summarize here. [Pg.68]

Using laser fluorescence measurements on fuel-rich H2/02/N2 flames seeded with H2S, Muller et al. [43] determined the concentrations of SH, S2, SO, S02, and OH in the post-flame gases. From their results and an evaluation of rate constants, they postulated that the flame chemistry of sulfur under rich conditions could be described by the eight fast bimolecular reactions and the two three-body recombination reactions given in Table 8.4. [Pg.448]

However, if it occurs, it appears to be minor. Thus, based on a review of the relevant studies reported in the literature, DeMore et al. (1997) suggest that k l0 = 4.5 X 10-l4e-1260/7 = 6.6 X 10 16 cm3 molecule 1 s 1 at 298 K. This can be compared to an effective second-order rate constant for reaction (9) at 1 atm of 1.3 X 10 12 cm3 molecule-1 s-1. In short, the two-body reaction is more than three orders of magnitude slower than the termolecular process at 1 atm pressure. [Pg.268]

In the epilimnion/hypolimnion two-box model the vertical concentration profile of a chemical adopts the shape of two zones with constant values separated by a thin zone with an abrupt concentration gradient. Often vertical profiles in lakes and oceans exhibit a smoother and more complex structure (see, e.g., Figs. 19.1a and 19.2). Obviously, the two-box model can be refined by separating the water body into three or more horizontal layers which are connected by vertical exchange rates. [Pg.999]

Thus a substantial body of experimental evidence shows that 1,2-disubstituted cyclopropanes, including vinylcyclopropanes, react thermally to give isomeric cyclopropanes through both one-center and two-center epimerizations, with (kt + k2) kl2 ratios from 1.4 to 4. Rate constants for both (, + k2) and kl2 events respond to the capacity of substituents to stabilize adjacent radicals in a regular fashion consistent with trimethylene diradical transition structures. Rate constants for vinylcyclopropane structural isomerizations do as well, thus reinforcing the notion that these reactions are nonconcerted diradical mediated reactions. [Pg.479]

In contrast, the need to evaluate the relative rates of competing radical reactions pervades synthetic planning of radical additions and cyclizations. Further, absolute rate constants are now accurately known for many prototypical radical reactions over wide temperature ranges.19,33 3S These absolute rate constants serve to calibrate a much larger body of known relative rates of radical reactions.33 Because rates of radical reactions show small solvent dependence, rate constants that are measured in one solvent can often be applied to reactions in another, especially if the two solvents are similar in polarity. Finally, because the effects of substituents near a radical center are often predictable, and because the effects of substituents at remote centers are often negligible, rate constants measured on simple compounds can often provide useful models for the reactions of complex substrates with similar substitution patterns. [Pg.722]

PK modeling can take the form of relatively simple models that treat the body as one or two compartments. The compartments have no precise physiologic meaning but provide sites into which a chemical can be distributed and from which a chemical can be excreted. Transport rates into (absorption and redistribution) and out of (excretion) these compartments can simulate the buildup of chemical concentration, achievement of a steady state (uptake and elimination rates are balanced), and washout of a chemical from tissues. The one- and two-compartment models typically use first-order linear rate constants for chemical disposition. That means that such processes as absorption, hepatic metabolism, and renal excretion are assumed to be directly related to chemical concentration without the possibility of saturation. Such models constitute the classical approach to PK analysis of therapeutic drugs (Dvorchik and Vesell 1976) and have also been used in selected cases for environmental chemicals (such as hydrazine, dioxins and methyl mercury) (Stem 1997 Lorber and Phillips 2002). As described below, these models can be used to relate biomonitoring results to exposure dose under some circumstances. [Pg.190]

Besides the splitting molecular oxygen out with the rate constant ka, ethyl peroxyl radicals may fragment (kb) to hydrogenperoxyl and ethylene. The ratio of rate constants ka/kb for these two alternatives is about 6 for excited ethyl peroxyl radicals at the value of ka 106 s 1. The rate constant for the deactivation of excited radicals with the third body M ... [Pg.203]


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