Butler–Volmer equation

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The Butler–Volmer equation is one of the most fundamental relationships in electrochemical kinetics. It describes how the electrical current on an electrode depends on the electrode potential, considering that both a cathodic and an anodic reaction occur on the same electrode:

 I = A \cdot j_0 \cdot \left\{ \exp \left[ \frac { \alpha_a nF } {RT} (E - E_{eq}) \right] - \exp \left[ - { \frac { \alpha_c nF } {RT}} (E - E_{eq}) \right] \right\}

or in a more compact form:

 j = j_0 \cdot \left\{ \exp \left[ \frac { \alpha_a nF \eta} {RT} \right] - \exp \left[ - { \frac { \alpha_c nF \eta} {RT}} \right] \right\}
Butler-Volmer dependence of the electrode current on overpotential η = E - Eeq. The anodic and cathodic current are shown as ia and ik, respectively. The total current i = ia + ik.

where:

The equation is named after chemists John Alfred Valentine Butler[1] and Max Volmer.

Mass-transfer control[edit]

The previous form of Butler–Volmer equation is valid when the electrode reaction is controlled by electrical charge transfer at the electrode (and not by the mass transfer to or from the electrode surface from or to the bulk electrolyte). Nevertheless, the utility of the Butler–Volmer equation in electrochemistry is wide, and it is often considered to be "central in the phenomenological electrode kinetics".[2]

In the region of the limiting current, when the electrode process is mass-transfer controlled, the value of the current density is:

i_{limiting} = \frac {nFD} {\delta} C^*

where:

  • D is the diffusion coefficient;
  • δ is the diffusion layer thickness;
  • C* is the concentration of the electroactive (limiting) species in the bulk of the electrolyte.
  • C(0,t) is the time-dependent concentration at the distance zero from the surface.

The above form simplifies to the conventional one (shown at the top of the article) when the concentration of the electroactive species at the surface is equal to that in the bulk.

The limiting cases[edit]

There are two limiting cases of the Butler–Volmer equation:

  • the low overpotential region (called "polarization resistance", i.e., when E ≈ Eeq), where the Butler–Volmer equation simplifies to:
i=i_0 \frac {nF} {RT} (E-E_{eq});
  • the high overpotential region, where the Butler–Volmer equation simplifies to the Tafel equation:
E-E_{eq} = a - b \log(i) for a cathodic reaction, when E << Eeq, or
E-E_{eq} = a + b \log(i) for an anodic reaction, when E >> Eeq

where a and b are constants (for a given reaction and temperature) and are called the Tafel equation constants. The theoretical values of a and b are different for the cathodic and anodic processes.

See also[edit]

References[edit]

  1. ^ Mayneord, W. V. (1979). "John Alfred Valentine Butler. 14 February 1899-16 July 1977". Biographical Memoirs of Fellows of the Royal Society 25: 144–126. doi:10.1098/rsbm.1979.0004.  edit
  2. ^ J. O'M. Bockris, A.K.N.Reddy, and M. Gamboa-Aldeco, "Modern Electrochemistry 2A. Fundamentals of Electrodics.", Second Edition, Kluwer Academic/Plenum Publishers, p.1083, 2000.