A simple and effective method for the accurate extraction of kinetic parameters using differential Tafel plots

The practice of estimating the transfer coefficient ([Formula: see text] ) and the exchange current ([Formula: see text] ) by arbitrarily placing a straight line on Tafel plots has led to high variance in these parameters between different research groups. Generating Tafel plots by finding kinetic current, [Formula: see text] from the conventional mass transfer correction method does not guarantee an accurate estimation of the [Formula: see text] and [Formula: see text] . This is because a substantial difference in values of [Formula: see text] and [Formula: see text] can arise from only minor deviations in the calculated values of [Formula: see text] . These minor deviations are often not easy to recognise in polarisation curves and Tafel plots. Recalling the IUPAC definition of [Formula: see text] , the Tafel plots can be alternatively represented as differential Tafel plots (DTPs) by taking the first order differential of Tafel plots with respect to overpotential. Without further complex processing of the existing raw data, many crucial observations can be made from DTP which is otherwise very difficult to observe from Tafel plots. These for example include a) many perfectly looking experimental linear Tafel plots (R(2) > 0.999) can give rise to incorrect kinetic parameters b) substantial differences in values of [Formula: see text] and [Formula: see text] can arise when the limiting current ([Formula: see text] ) is just off by 5% while performing the mass transfer correction c) irrespective of the magnitude of the double layer charging current ([Formula: see text] ), the Tafel plots can still get significantly skewed when the ratio of [Formula: see text] is small. Hence, in order to determine accurate values of [Formula: see text] and [Formula: see text] , we show how the DTP approach can be applied to experimental polarisation curves having well defined [Formula: see text] , poorly defined [Formula: see text] and no [Formula: see text] at all.