Hydrogen overpotentials on metal cathodes

Potentials and overpotentials of 11 cathodes measured by Tafel in 1905 in 2 N sulfuric acid at about 12 °C and 0.1 A/cm², with the extra energy the overpotential costs per mole of H₂.

11 rows
Hg\ce{Hg}—1.9741.30251—
Pb\ce{Pb}polished1.9701.30251—
Pb\ce{Pb}rough1.9001.23237—
Cd\ce{Cd}—1.8901.22235—
Sn\ce{Sn}—1.8201.15222—
Bi\ce{Bi}—1.6701.00193—
Au\ce{Au}—1.6200.95183—
Ag\ce{Ag}—1.6000.93179queried in the original
Cu\ce{Cu}—1.4600.79152—
Ni\ce{Ni}—1.4100.74143—
Pt\ce{Pt}platinised0.7450.0714—

η = ε − 0.674 V (the reversible hydrogen electrode against mercury–mercurous sulfate in 2 N sulfuric acid). Values are time-maximum readings at constant current; on copper, nickel and gold the potential drifted for hours and is less reliable. Overpotentials change with current density, temperature and surface condition.

Sources

  1. J. Tafel, “Über die Polarisation bei kathodischer Wasserstoffentwicklung”, Z. Phys. Chem. 50, 641–712 (1905), Table 12 and p. 655.

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