Reaction Kinetics: Reactions in Solution
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Reaction Kinetics - Keith J. Laidler
LAIDLER
CHAPTER 1
Reactions in Solution: General Principles
Publisher Summary
Liquids neither have a completely random nor a completely regular structure, and their theoretical treatment is consequently much more complicated. It is, therefore, necessary to proceed in a less fundamental and more empirical fashion than is possible in the case of gas reactions or of reactions in solids or on solid surfaces in dealing with reactions in solution. Despite that, much valuable knowledge has accumulated regarding reactions in solution, particularly for certain classes of reactions. Reactions in solution are of a variety of types. There are certain reactions for which the solvent plays a relatively subsidiary role; it seems to act as a mere space-filler and has only a minor influence on the rate of reaction. Such reactions are little affected by a change in solvent and occur in the gas phase at much the same rate as in solution. An example of such a reaction is the thermal decomposition of nitrogen pentoxide.
The liquid state is not understood in anything like the same detail as the gaseous and solid states. In the gaseous state the interactions between individual molecules are usually relatively un-important; the molecules therefore behave largely in a random manner and can be treated in terms of the kinetic theory, which deals with such randomness. Solids, having a regular structure, can also be treated in a satisfactory manner. Liquids, on the other hand, have neither a completely random nor a completely regular structure, and their theoretical treatment is consequently very much more complicated. It is therefore necessary, in dealing with reactions in solution, to proceed in a less fundamental and more empirical fashion than is possible in the case of gas reactions or of reactions in solids or on solid surfaces. In spite of this, much valuable knowledge has accumulated regarding reactions in solution, particularly for certain classes of reactions.
Reactions in solution are of a variety of types. There are certain reactions for which the solvent plays a relatively subsidiary role; it seems to act as a mere space-filler and has only a minor influence on the rate of reaction. Such reactions are little affected by a change in solvent, and occur in the gas phase at much the same rate as in solution. An example of such a reaction is the thermal decomposition of nitrogen pentoxide, some data(1) for which are given in Table 1. The rate constants, frequency factors and activation energies are seen to be very much the same in the solvents mentioned and in the gas phase. In nitric acid solution, on the other hand, the rate constant is significantly lower (0·147 × 10−5 at 25°C) and the activation energy higher (28·3 kcal per mole), indicating that this solvent plays a more active role in the reaction.
TABLE 1
The Decomposition of Nitrogen Pentoxide
Those solvents that have no effect on rates, frequency factors and activation energies probably do not interact very much with the reactant molecules or the activated complexes. An important question that arises in such cases is the frequency of collisions between solute molecules, as compared with the frequency in the gas phase. This matter has been treated theoretically both from the point of view of the kinetic theory of collisions and of the absolute rate theory. A collision theory approach was employed by Rabinowitch(1), who based his treatment on a theoretical study made in 1930 by Debye and Menke of the structure of liquid mercury. Mercury is a very simple liquid, the particles being atoms, and the arrangement of the atoms in the liquid is comparatively regular. Using a distribution function for mercury given by Debye and Menke, Rabinowitch calculated the frequency of collisions between a given pair of mercury atoms, and compared this frequency with the frequency in the gas phase. His conclusion was that in the liquid the frequency of collisions is approximately two to three times greater than that in the gas phase.
The theory of absolute reaction rates was applied to this problem by M. G. Evans and M. Polanyi(1), and also by R. P. Bell(2). Since it is not possible to write down satisfactory partition functions for molecules in the liquid phase (because of the complicated nature of their translational, rotational and vibrational motions) it is more convenient to apply the theory of absolute reaction rates in terms of entropies of activation rather than of partition functions. In Bell’s treatment empirical values for entropies of non-polar molecules in solution were employed, and from them were estimated the entropies of activation for reactions involving such molecules. In agreement with collision theory, his conclusion was that the frequency factor for a reaction in solution should be approximately three times as great as in the gas phase. On the assumption that the energies of activation are the same in solution and in the gas phase, both the collision theory and the theory of absolute reaction rates would therefore indicate that the rates in solution should be approximately three times as great as in the gas