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Electrode Polarisations  2 39

                 point some distance away from the TPB. Thus, many possibilities exist
                 wherein there are a number of  possible parallel steps to the net charge
                 transfer  reaction.  Experimental  work  combined  with  continnum
                 modeling has been conducted in order to analyse various reaction steps
                 [15,17,20,2 11; experimental  methods  used  in  these  studies  include
                 steady-state  current-voltage  characteristics  and  electrochemical
                 impedance  spectroscopy.  The  importance  of  the  role  of  TPB  in
                 Lal,(Sr,Ca),Mn03   and  Lal-$r,Mn03   cathodes  is  documented  in
                 appended references [14,20,22,23]. These studies showed that oxygen
                 reduction predominantly occurs at TPB’s when these materials are used
                 as cathodes. However, bulk transport of  oxygen through Lal-,Sr,MnO3
                 has been reported under high applied overpotentials [9]. A wide variety of
                 reaction mechanisms have been proposed in the literature, even using
                 nominally  similar  electrode  materials.  This  lack  of  consistency  is
                 apparently due to the fact that electrode processes and morphology are
                 closely interrelated, and also that the fundamental mechanisms are not
                 fully understood at the present time. Considering that the current and
                 potential  distribution  in  the  3-dimensional  porous  system  and  the
                 available  reaction  zone  both  depend  on  the  microstructure  and  the
                 presence of  secondary phases and impurities at the interface, it is clear
                 that a simple, unified reaction mechanism is unrealistic. But this in large
                 part is also due to a lack of a quantitative characterisation  of  electrode
                 microstructure,  and a Iack of  quantitative analysis of  the relationship
                 between microstructure and cathode performance. Such a quantitative
                 study has been reported in only a limited number of studies, such as those
                 by Zhao et al. [24] and Weberet al. [25].
             Above reactions 1) to 4) describe a number of possible, series steps, and in the
           simplest model, the slowest one is the rate-determining step4. The remaining
           steps then can be assumed to be close to equilibrium. Many of the above steps are
           generally  thermally  activated.  The  rate  of  cathodic  reaction  is  directly
           proportional to the net current density: or more precisely, the net current density
           is proportional to the cathodic reaction rate. Associated with the reaction rate, or
           the passage of current, is a loss in voltage, which is the activation polarisation or
           overpotential;  the  terminology  being  derived  from  the  thermally  activated
           nature  of  the  reaction.  The  relationship  between  the  cathodic  activation
           polarisation, Y&~, and the current density is usually nonlinear, except at very low
           current densities. In general,

               r&t  = f(materia1 properties, microstructure, temperature,
                      atmosphere, current density)                           (16)
              It is to be emphasised that it is not necessary that there be a single rate-determining step. If two or
           more steps exhibit similar kinetic barriers, it is quite possible that a simple dependency of the so-called
           rate-determining step on a given parameter (e.g. oxygen partial pressure) will not be reflected in the
           overall measured effect. That is, there can be more than one step away from equilibrium The analysis of
           data in such a case can be particularly difficult.
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