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Totally irreversible systems

This system represented a somewhat less formidable problem than quasi-reversible charge transfer [15]. The surface flux equation is given by [Pg.154]

The rate constant in the reverse direction is considered to be insignificant for these systems. The numerical solution of the appropriate integral equation led to [Pg.154]


Irreversible and Quasi-Reversible Systems For irreversible processes (those with sluggish electron exchange), the individual peaks are reduced in size and widely separated (Figure 2-5, curve A). Totally irreversible systems are characterized by a shift of the peak potential with the scan rate ... [Pg.32]

For irreversible systems the peak potential of a reduction process is shifted toward more negative potentials by about 0.030 V for a decade increase in the scan rate [Eq. (3.43)]. By analogy, a peak of an anodic process is shifted toward more positive potentials. The most characteristic feature of a cyclic voltammogram of a totally irreversible system is the absence of a reverse peak. However, it does not necessarily imply an irreversible electron transfer but could be due to a fast following chemical reaction. [Pg.75]

An electrochemical process such as A + ne P is said to be reversible if the Nernst equation is obeyed under the conditions of the experiment. In a totally irreversible system, either the forward or the reverse reaction is so slow as to be completely negligible. In a partially reversible system, the reaction in one direction is much slower than the other, but not totally insignificant. A process that appears reversible on a slow time scale may show signs of irreversibility when the time scale of the experiment is increased. [Pg.678]

As a prelude to a treatment of steady-state voltammetry in quasireversible and totally irreversible systems, it is useful to develop a very general description of current flow in a step experiment at a spherical electrode. In Section 5.4.2(a) the basic diffusion problem was outlined, and the following relationships arose without invoking a particular kinetic condition. [Pg.197]

When the wave is not reversible, the half-wave potential is not a good estimate of the formal potential and cannot be used directly to determine thermodynamic quantities in the manner discussed in Section 5.4.4. In the case of a totally irreversible system, the wave shape and position can furnish only kinetic information, but quasireversible waves can... [Pg.201]

If the electrode process is more complex than the one-step, one-electron model (e.g., n> with a rate-determining heterogeneous electron transfer), then the wave shape can become extremely difficult to analyze. An exception is the case where the initial step is the rate-determining electron transfer [Section 3.5.4(b)], in which case all that has been discussed for totally irreversible systems also applies, but with the current multiplied consistently by n. [Pg.202]

Tomes criterion and half-wave potential. As one can see from Table 5.5.1, 3/4 — 1/4 for a totally irreversible system provides a directly. That figure can then be used in conjunction with (5.5.30) [for early transients] or 5.5.49 [for steady-state voltammetry] to obtain l. Butler-Volmer kinetics are implicit and E must be known. [Pg.203]

Curve fitting. This method applies to voltammetry based on either transient or steady-state currents and proceeds essentially exactly as described for totally irreversible systems, except that the fitting function must be developed from (5.5.24) or (5.5.44). [Pg.204]

Equation 5.5.28 for early transients in a totally irreversible system having only species O present in the bulk. [Pg.223]

Koutecky treated the totally irreversible system at the DME and expressed the result as (29, 30)... [Pg.273]

Since a is usually between 0.3 and 0.7, both the wave slope and the Tomes criterion for a totally irreversible system are normally significantly larger than for a reversible system. These figures of merit are not without ambiguity, however. Consider the predicted wave slope of 63.8 mV for a = 0.85. Within the precision of normal measurements, one could diagnose the system as either reversible or irreversible. It is always a good idea to examine reversibility by a method, such as cyclic voltammetry, that allows a view of the electrode reaction in both directions. [Pg.274]

Table 6.2 - Diagnostic tests for totally irreversible systems at 25°C... Table 6.2 - Diagnostic tests for totally irreversible systems at 25°C...
Although the cyclic voltammograms appear to be irreversible, they should not be. In the case of a totally irreversible system, we cannot expect to determine the reduction potential. To understand this apparent anomaly more fully, a study of the reversibility of the system was performed. The electrochemical current corresponds to the difference between the rate of the forward electron transfer kf[Bi2a] and its rate kb[Bi2a] for the reverse process. The reversibility factor f, for the methylcobalamin system is described as follows ... [Pg.144]


See other pages where Totally irreversible systems is mentioned: [Pg.1928]    [Pg.154]    [Pg.160]    [Pg.268]    [Pg.201]    [Pg.202]    [Pg.234]    [Pg.235]    [Pg.1928]    [Pg.30]    [Pg.46]    [Pg.144]    [Pg.24]    [Pg.44]    [Pg.423]   


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