Physical Chemistry Third Edition

(C. Jardin) #1

13.5 Nonequilibrium Electrochemistry 607


Butler–Volmer equation, Eq. (13.5-22), is much larger than the first term, and

|j|≈j 0 e−αnF η/RT (13.5-24)

Solving this equation forηgives

η

RT

αnF

ln(j 0 )−

RT

αnF

ln(|j|) (13.5-25)

Equation (13.5-25) is of the form of theTafel equation, an empirical equation of
the form

|η|a+blog 10 (|j|) (13.5-26)

The reduction of hydrogen ions at various metal electrode surfaces has been exten-
sively studied. The mechanism of the electrode reaction can depend on the material of
the electrode. One possible mechanism is^33

(1) H++e−+MM−H (13.5-27a)
(2) 2 M−H−→2M+H 2 (13.5-27b)

where M denotes the metal of the electrode, and M−H denotes a chemically adsorbed
hydrogen atom. Another possible mechanism is^34

(1) H++e−+MM−H (13.5-28a)
(2) M−H+H++e−−→M+H 2 (13.5-28b)

In either of these mechanisms, it is possible for different metals that either the first step
or the second step is rate-limiting. If the first step of the mechanism of Eq. (13.5-27) is
rate-limiting in both directions,

(forward rate)k 1 [H+]G(1−θ) (13.5-29)

where [H+]Gdenotes the concentration of hydrogen ions at the Guoy plane (outer
Helmholtz plane) andθdenotes the fraction of surface sites occupied by hydrogen
atoms. If the electric potential in the bulk of the solution is called zero, then by the
Boltzmann probability distribution

[H+]G[H+]be−Fφ^1 /RT (13.5-30)

where [H+]bdenotes the concentration of H+in the bulk of the solution and whereφ 1
is the electric potential at the Guoy plane.
The rate at equilibrium gives the exchange current. Using Eq. (13.5-13a) for the rate
constant,

j 0 F(1−α)[H+]bexp

[

−Fφ 1
RT

]

k◦exp

[

( 1 −α)nF(φ−φ◦)
RT

]

(13.5-31)

With the expression in Eq. (13.5-31) for the exchange current, the Butler–Volmer
equation, Eq. (13.5-22), and Eqs. (13.5-23) through (13.5-25) can be used, since it is
of the same form for a reduction as for an oxidation half-reaction.

(^33) K. J. Laidler,J. Chem. Educ., 47 , 600 (1970) (note 1).
(^34) Ibid.

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