1960
DOI: 10.1149/1.2427580
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Erratum: “Theory of Faradaic Distortion” [J. Electrochem. Soc., 107, 768 (September 1960)]

Abstract: not Available.

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“…The starting potential typically corresponds to a condition of zero current. It is convenient to classify a step to the final potential as either a “potential perturbation” or a “potential leap.” The former constitutes relatively small amplitude steps to potentials less than those required to produce a transport-limited current under steady-state conditions. The latter corresponds to a large amplitude jump to a final potential corresponding to a steady-state transport-limited current.…”
Section: Introductionmentioning
confidence: 99%
“…The starting potential typically corresponds to a condition of zero current. It is convenient to classify a step to the final potential as either a “potential perturbation” or a “potential leap.” The former constitutes relatively small amplitude steps to potentials less than those required to produce a transport-limited current under steady-state conditions. The latter corresponds to a large amplitude jump to a final potential corresponding to a steady-state transport-limited current.…”
Section: Introductionmentioning
confidence: 99%
“…This expression is obtained through the linearization of the Butler-Volmer equation for a small overpotentiaI. 2 5 In the derivation of the expressions for this equivalent circuit, small ac signal conditions are assumed to be met, so that non-linear behaviour, such as Faraday distortion 26 and rectification,27 is avoided.…”
Section: Z Fsl 3zfsdmentioning
confidence: 99%