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The Tafel Equation: When the Reverse Reaction Can Be Ignored

The Butler–Volmer equation contains two terms: one for oxidation and one for reduction. Close to equilibrium both matter, but a little way from it the reverse reaction becomes so slow that it can be ignored. The equation then simplifies to the Tafel equation, and a plot of log |i| against η becomes a straight line from which the exchange current density can be read. Work through the three stages in order.

Predict, then see:

Or explore freely:

0.000 V

  • The dashed curves are the two terms of the Butler–Volmer equation: orange for oxidation, blue for reduction. The solid curve is their sum, the net current.
  • The bar under the graph compares the reverse reaction with the forward one. Once it is below 1 %, the reverse term can be ignored: this is the Tafel region.

Remember

  • Butler–Volmer: i = i0[eαnFη/RT − e−(1−α)nFη/RT]. With α = 0.5 the reverse term is a fraction e−nF|η|/RT of the forward term.
  • The reverse reaction falls below 1 % of the forward reaction when |η| > 0.118 V/n: 0.12 V for n = 1 and 0.06 V for n = 2.
  • Beyond this point (the Tafel region) only one term remains. For reduction, |i| = i0e(1−α)nF|η|/RT; taking logarithms gives the Tafel equation, |η| = b log(|i|/i0).
  • Tafel slope: b = 2.303RT/(αnF), the extra overpotential needed for each tenfold increase in current. With α = 0.5 at 298 K: 118 mV per decade for n = 1, 59 mV per decade for n = 2.
  • On a Tafel plot (log |i| against η), the straight line extrapolated back to η = 0 meets the axis at log i0.

Exchange current densities are those in the Lecture 5 and 6 tables. The value of n in the exponent is the number of electrons in the half-reaction, as in the lecture examples, and α = 0.5 throughout.