The anodic polarization process in metal-hydride electrodes occurs via the
following consecutive steps: (i) diffusion of absorbed hydrogen from the bu
lk to the surface of the electrode, (ii) hydrogen transfer from absorbed st
ate to adsorbed state at the electrode surface, and (iii) electrochemical o
xidation of the adsorbed hydrogen on the electrode surface. A theoretical t
reatment is presented to account for the dependencies on these three consec
utive steps, of the reaction resistances, anodic limiting current, cathodic
limiting current, and exchange current. The theoretical analysis predicts
that the total resistances measured from linear micropolarization is the su
m of the charge-transfer, hydrogen-transfer, and hydrogen-diffusion resista
nces, which is in contradiction with the generally accepted idea that the r
esistance measured from linear micropolarization is only the charge-transfe
r resistance. For a metal-hydride electrode with a flat pressure plateau at
a low state of discharge (SOD), the resistance measured from linear microp
olarization is approximately equal to the sum of three resistances measured
from AC impedance, namely, charge-transfer, hydrogen-transfer and hydrogen
-diffusion resistances; however, when the SOD is high, the resistance measu
red from linear micropolarization is higher than total resistances measured
from AC impedance. (C) 2000 Elsevier Science S.A. All rights reserved.