Pure and Applied Chemistry· 2014Q3
Defining the transfer coefficient in electrochemistry: An assessment (IUPAC Technical Report)
- 518citations
- Q3SCImago
- 2014year
Short summary
This IUPAC technical report redefines the transfer coefficient (α) in electrochemistry to be independent of mechanistic assumptions, proposing αc = –(RT/F)(d ln|jc|/dE) and αa = (RT/F)(d ln ja/dE). The current definitions are shown to apply only to single-electron transfer elementary steps, which are rare, and their uncritical application leads to erroneous mechanistic interpretations.
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Key points
- Existing definitions of cathodic (αc) and anodic (αa) transfer coefficients are restricted to single-step, multi-electron elementary reactions.
- The simultaneous transfer of multiple electrons in a single elementary step is considered highly improbable based on absolute rate theory.
- Uncritical application of current definitions leads to misinterpretations of electrode reaction mechanisms, particularly when estimating the number of electrons (n).
- The proposed new definitions, αc = –(RT/F)(d ln|jc|/dE) and αa = (RT/F)(d ln ja/dE), are independent of mechanistic assumptions.
AI-generated from the title and abstract; the full text is not read.
Abstract
Abstract The transfer coefficient α is a quantity that is commonly employed in the kinetic investigation of electrode processes. In the 3 rd edition of the IUPAC Green Book, the cathodic transfer coefficient α c is defined as –( RT / nF )( d ln k c /d E ), where k c is the electroreduction rate constant, E is the applied potential, and R, T , and F have their usual significance. This definition is equivalent to the other, -( RT / nF )( d ln| j c |/d E ), where j c is the cathodic current density corrected for any changes in the reactant concentration at the electrode surface with respect to its bulk value. The anodic transfer coefficient α a is defined similarly, by simply replacing j c with the anodic current density j a and the minus sign with the plus sign. It is shown that this definition applies only to an electrode reaction that consists of a single elementary step involving the simultaneous uptake of n electrons from the electrode in the case of α c , or their release to the electrode in the case of α a . However, an elementary step involving the simultaneous release or uptake of more than one electron is regarded as highly improbable in view of the absolute rate theory of electron transfer of Marcus; the hardly satisfiable requirements for the occurrence of such an event are examined. Moreover, the majority of electrode reactions do not consist of a single elementary step; rather, they are multistep, multi-electron processes. The uncritical application of the above definitions of α c and α a has led researchers to provide unwarranted mechanistic interpretations of electrode reactions. In fact, the only directly measurable experimental quantity is d ln| j |/d E , which can be made dimensionless upon multiplication by RT / F , yielding ( RT / F )( d ln| j |/d E ). One common source of misinterpretation consists in setting this experimental quantity equal to αn , according to the above definition of the transfer coefficient, and in trying to estimate n from αn , upon ascribing an arbitrary value to α , often close to 0.5. The resulting n value is then identified with the number of electrons involved in a hypothetical rate-determining step or with that involved in the overall electrode reaction. A few examples of these unwarranted mechanistic interpretations are reported. In view of the above considerations, it is proposed to define the cathodic and anodic transfer coefficients by the quantities α c = –( RT / F )( d ln| j c |/d E ) and α a = ( RT / F )( d ln j a /d E ), which are independent of any mechanistic consideration.
The authors' abstract, as published at the source. Pure and Applied Chemistry, 2014 · DOI ↗
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Field: Electrochemistry
ElectrochemistryChemistry