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Essentials of Computational Chemistry

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15<br />

Adiabatic Reaction Dynamics<br />

15.1 Reaction Kinetics and Rate Constants<br />

Consider an arbitrary equilibrium system<br />

A + B + C +···−−−⇀<br />

↽−−− ···+X + Y + Z (15.1)<br />

where no particular stoichiometry is implied. When the system is displaced from equilibrium,<br />

by addition <strong>of</strong> more <strong>of</strong> a particular species, by a change in temperature and/or pressure, or<br />

by any other influence, empirical observation has shown that the rate at which equilibrium<br />

is reestablished may be expressed as<br />

rate(t) = kφ(t) [A]a [B] b [C] c ···<br />

···[X] x [Y] y [Z] z<br />

(15.2)<br />

where kφ is a phenomenological rate constant (distinguished from an elementary rate constant<br />

as defined later on), [W] represents the concentration <strong>of</strong> species W (usually expressed in<br />

units <strong>of</strong> molarity or partial pressure), and each concentration term has associated with it an<br />

exponent that is sometimes referred to as the ‘molecularity’ <strong>of</strong> the species. Often, but not<br />

always, molecularities have integral values, including zero. Note that since we are measuring<br />

a return to equilibrium, all concentration terms are functions <strong>of</strong> time t, asarekφ and the rate<br />

itself.<br />

The apriori prediction <strong>of</strong> all <strong>of</strong> the variables appearing on the r.h.s. <strong>of</strong> Eq. (15.2) is<br />

a challenging task, to say the least. This is particularly true because the equilibrium <strong>of</strong><br />

Eq. (15.1) may involve the simultaneous operation <strong>of</strong> a large number <strong>of</strong> individual chemical<br />

reactions, with some possibly involving very low concentrations <strong>of</strong> reactive intermediates,<br />

the presence <strong>of</strong> which may be difficult to establish experimentally. In order to make progress,<br />

a critical simplification is to break the overall process down into so-called elementary steps.<br />

To simplify matters a bit, we will consider only adiabatic reaction steps, that is, reactions<br />

taking place on a single PES without any change in electronic state (the topic <strong>of</strong> non-adiabatic<br />

dynamics is discussed briefly in Section 15.5). For practical purposes, there are only two<br />

kinds <strong>of</strong> elementary reactions: unimolecular and bimolecular.<br />

<strong>Essentials</strong> <strong>of</strong> <strong>Computational</strong> <strong>Chemistry</strong>, 2nd Edition Christopher J. Cramer<br />

© 2004 John Wiley & Sons, Ltd ISBNs: 0-470-09181-9 (cased); 0-470-09182-7 (pbk)

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