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ELECTROCHEMICAL METHODS Fundamentals and Applications - Allen.J.Bard

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30 • Chapter 1. Introduction <strong>and</strong> Overview of Electrode Processes<br />

C o<br />

(x =<br />

Figure 1.4.1 Concentration profiles (solid lines) <strong>and</strong> diffusion layer approximation (dashed<br />

lines), x = 0 corresponds to the electrode surface <strong>and</strong> 8 0<br />

is the diffusion layer thickness.<br />

Concentration profiles are shown at two different electrode potentials: (7) where C 0<br />

(x = 0)<br />

is about CQ/2, (2) where C 0<br />

(x = 0) « 0 <strong>and</strong> i = i h<br />

Since 8Q is often unknown, it is convenient to combine it with the diffusion coefficient to<br />

produce a single constant, YHQ — DQ/8Q, <strong>and</strong> to write equation 1.4.4 as<br />

~ C o<br />

(x = 0)] (1.4.5)<br />

The proportionality constant, m o<br />

, called the mass-transfer coefficient, has units of<br />

cm/s (which are those of a rate constant of a first-order heterogeneous reaction; see<br />

Chapter 3). These units follow from those of v <strong>and</strong> CQ, but can also be thought of as<br />

volume flow/s per unit area (cm 3 s" 1 cm" 2 ). 11 Thus, from equations 1.4.1 <strong>and</strong> 1.4.5<br />

<strong>and</strong> taking a reduction current as positive [i.e., / is positive when CQ > CQ(X = 0)], we<br />

obtain<br />

nFA = m o[C% - C o<br />

(x = 0)] (1.4.6)<br />

Under the conditions of a net cathodic reaction, R is produced at the electrode surface, so<br />

that C R<br />

(x = 0) > CR (where CR is the bulk concentration of R). Therefore,<br />

= m R<br />

[C R<br />

(x = 0) - C*] (1A7)<br />

11<br />

While m 0<br />

is treated here as a phenomenological parameter, in more exact treatments the value of m 0<br />

can<br />

sometimes be specified in terms of measurable quantities. For example, for the rotating disk electrode,<br />

m 0<br />

= 0.62D /3 o<br />

(o l/2 v~ l/e , where со is the angular velocity of the disk (i.e., 2тг/, with/as the frequency in<br />

revolutions per second) <strong>and</strong> v is the kinematic viscosity (i.e., viscosity/density, with units of cm 2 /s) (see<br />

Section 9.3.2). Steady-state currents can also be obtained with a very small electrode (such as a Pt disk<br />

with a radius, r 0<br />

, in the \xva range), called an ultramicroelectrode (UME, Section 5.3). At a disk UME,<br />

m 0<br />

= 4D o<br />

/7rr 0<br />

.

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