1981
DOI: 10.1139/v81-370
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Internal energy randomisation in weak-collision unimolecular reaction systems

Abstract: H. 0. PRITCHARD and S. R. VATSYA. Can. J. Chem. 59, 2575 (1981). We examine the conjecture that the principal difference between weak-collision and strong-collision behaviour in thermal unimolecular reaction systems arises from a difference in internal energy randomisation rates. To do this, we solve analytically the strong-collision master equation for a thermal unimolecular reaction including explicit allowance for the randomisation processes, and we show that all weak-collision effects so far observed in th… Show more

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Cited by 12 publications
(3 citation statements)
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“…Determination of the limits of yo with p , p, is much simpler than before, by direct expansion of [8] and/or [9], but the results are the same as those given previously (1).…”
Section: Mathematical Preliminariesmentioning
confidence: 87%
“…Determination of the limits of yo with p , p, is much simpler than before, by direct expansion of [8] and/or [9], but the results are the same as those given previously (1).…”
Section: Mathematical Preliminariesmentioning
confidence: 87%
“…For a given set of initial conditions and a given value of the conserved ratio Fcl/FBr, we shall denote a quasi-steady state that is characterized by = 1.0 by the letter A, one that has ^1.0 but does not persist to equilibrium by B, and one that has y± 1.0 but does persist to equilibrium by C. As an example, we refer to the first, second, and third quasi-steady states of run 12 in Table III as quasi-steady states of types A, B, and C respectively. In quasi-steady state B,, all components of dcij (j = 0, .... 16) remain constant to at least two significant figures. 6In quasi-steady state B2 not all components of dC2J (j = 0, .... 16) remain constant.…”
Section: "C1 = [Hc1]/[rp]mentioning
confidence: 97%
“…It was shown recently that the placing of a bottleneck in the activation process for a thermal unimolecular reaction could lead to the occurrence of strict Lindemann behaviour in the fall-off (I); it has also been found that if the randomisation processes become rate-limiting, strict Lindemann behaviour likewise ensues (2). Since several weak-collision thermal systems exhibit fall-off behaviour which is very close indeed to strict Lindemann (3), it is important to decide whether such behaviour may result from a bottleneck in the activation ladder or from a bottleneck in the randomisation process (or, perhaps, a combination of both).…”
Section: Introductionmentioning
confidence: 99%