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Pure and Applied Chemistry· 2014Q3

Defining the transfer coefficient in electrochemistry: An assessment (IUPAC Technical Report)

Rolando Guidelli, Richard G. Compton, Juan M. Feliú, E. Gileadi et al.

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.

AI-generated from the title and abstract; the full text is not read.

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