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Quasi-homogeneous substrate surface approach

In this simplest approach, following the concept of Delahay [3.305, 3.306] and Parsons [3.307], all adsorption sites of S are considered to be energetically equal. It is further assumed that localized adsorption of and desorption of Me Jg takes place [Pg.102]

Assuming y = z (no cosorption or competitive adsorption phenomena), the flux j(t) is related to the overall current density, i, by [Pg.102]

The potential dependence of both terms Aads and ifdes is described by the well-known Butler-Volmer equation [3.308, 3.309]. Both terms involve the exchange current density, s/j g +  [Pg.102]

Sign convention cathodic currents are taken to be negative [Pg.102]

39) describes r(E,f) changes under any polarization conditions (small and large signal system perturbation). [Pg.103]


Experimental results on the basis of a kinetic approach of Me UPD on quasi-homogeneous substrate surfaces using large and small signal system perturbation techniques are rather rare [3.89, 3.119, 3.214-3.216, 3.313, 3.314]. [Pg.105]

These controversial results on the kinetics of Me UPD processes, obtained on the basis of the simplest approach assuming quasi-homogeneous substrate surfaces, led to the development of a different kinetic model including surface inhomogeneities, gradients of Meads> and surface diffusion as discussed in the following. [Pg.107]


See other pages where Quasi-homogeneous substrate surface approach is mentioned: [Pg.102]    [Pg.102]    [Pg.921]   


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Quasi-homogeneous surface approach

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Surface homogeneity

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