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Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

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6 ELECTROCHEMICAL METHODS 157tant step was the transfer <strong>of</strong> H+ to the alcohol. The reaction is also significant inbeing the first very fast dissociation reaction <strong>of</strong> a strong acid whose kinetics havebeen measured.6. Electrochemical methodsIn suitable cases one <strong>of</strong> this family <strong>of</strong> techniques may be used to follow fastreactions in solution. They may be appropriate if one <strong>of</strong> the reactants is electrochemicallyreduced under conditions where the others are not. In the normal electrolyticreduction process a potential difference is applied between two electrodesplaced in the conducting solution, resulting in the migration <strong>of</strong> ions towards theelectrodes and the discharge at the cathode <strong>of</strong> that species which is most easilyreduced-i.e.,X+e- -+ A (in this section, the electroreduced species will be giventhe symbol X and other species will be represented by A, B, . . .). Because <strong>of</strong> thedischarge <strong>of</strong> X at the electrode a concentration gradient is set up between the bulk<strong>of</strong> the solution and the surface <strong>of</strong> the cathode. The current flowing is proportionalto the rate at which X is reduced. This can be expressed mathematically in terms <strong>of</strong>measurable quantities-an exercise which is greatly simplified if certain conditionsare obeyed. In the first place, the species X, which may be an ion, a molecule or afree radical, must be discharged “immediately” on arriving at the cathode; in otherwords, the discharge process should not be the rate-limiting step. Secondly, it is ahelp if the cathode is <strong>of</strong> a shape whose surface area may be simply expressed mathematically-e.g.,a sphere or an “infinite” plane. The third simplifying conditionis that the mass transfer from the bulk <strong>of</strong> the solution to the electrode surface be<strong>of</strong> one or, at most, two types. Three types may be considered: diffusion down aconcentration gradient, general convectional motion and movement down or up apotential gradient. The latter is no problem for uncharged X, but it can also beeffectively eliminated in the case <strong>of</strong> ions by using a large excess <strong>of</strong> an “inert” electrolytesuch as potassium chloride to carry the current in the bulk <strong>of</strong> the solution.These “inert” ions are not discharged at the electrodes until most <strong>of</strong> the specieswith smaller electrode potentid has been discharged. Typically, the conditions arechosen so that the limiting physical process in the electrolysis is diffusion down theconcentration gradient. A current which is characteristic <strong>of</strong> the system is measured,called the “diffusion current”.Now, suppose that the species which is discharged (the depolarizer) is involvedin an equilibrium <strong>of</strong> the typeX+BsC (7)<strong>of</strong> which the equilibrium constant is considerably greater than unity. Again a concentrationgradient is set up but, if the dissociation <strong>of</strong> C into X and B is slowerReferences pp. 176-1 79

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