Journal of Applied Electrochemistry

, Volume 23, Issue 6, pp 597–605

Temperature dependence of the Tafel slope for oxygen reduction on platinum in concentrated phosphoric acid

Authors

  • S. J. Clouser
    • Case Center for Electrochemical Sciences and the Department of ChemistryCase Western Reserve University
  • J. C. Huang
    • Case Center for Electrochemical Sciences and the Department of ChemistryCase Western Reserve University
  • E. Yeager
    • Case Center for Electrochemical Sciences and the Department of ChemistryCase Western Reserve University
Papers

DOI: 10.1007/BF00721951

Cite this article as:
Clouser, S.J., Huang, J.C. & Yeager, E. J Appl Electrochem (1993) 23: 597. doi:10.1007/BF00721951

Abstract

Oxygen reduction on bright platinum in concentrated H3PO4 has been investigated with the rotating disc electrochemical technique at temperatures from 25 to 250° C and oxygen pressures up to 1.77 MPa. Cyclic voltammetry has been employed to study the anodic film formed on platinum in concentrated H3PO4 and the possible electroreduction of H3PO4 on platinum. The apparent transfer coefficient for the oxygen reduction has been found to be approximately proportional to temperature rather than independent of temperature. Such behaviour is difficult to reconcile with accepted theories for the effect of electrode potential on the energy barriers for electrode processes. It is of importance to establish an understanding of this phenomenon. Possible factors which can contribute to the temperature dependence of the transfer coefficient but which would not necessarily result in a direct proportionality to temperature include potential dependent adsorption of solution phase species, restructuring of the solution in the compact layer, proton and electron tunnelling, a shift in rate-determining step, changes in the symmetry of the potential energy barrier, penetration of the electric field into the electrode phase, insufficient correction for ohmic losses, and impurity effects.

Nomenclature

α

transfer coefficient

β

symmetry factor

β′

temperature independent component of β

ν

stoichiometric number

ω

rotation rate (r.p.m.)

a,c

constant and temperature coefficient in Equation 4 (no unit and K−1, respectively)

B

slope of Koutecky-Levich plot (mA cm−2 (r.p.m.)1/2)

b

Tafel slope (V dec.−1)

E

potential (V)

F

Faraday (C mol−1)

i

current density (A cm−2)

iL

diffusion limiting current density (A cm−2)

K

temperature independent component of Tafel slope (V dec−1.)

R

gas constant (J mol−1 K−1)

T

temperature (K)

n

number of electrons

\((^{\ddag } ){\rm O}\)

standard free energy of activation for forward process (J mol−1)

\((^{\ddag } ){\rm O}\)

standard enthalpy of activation for forward process (J mol−1)

\((^{\ddag } ){\rm O}\)

standard entropy of activation for forward process (J mol−1 K−1)

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Copyright information

© Chapman & Hall 1993