Page 343 - High Temperature Solid Oxide Fuel Cells Fundamentals, Design and Applications
P. 343

Cell, Stuck and System Modelling  319

              In principle, one could make a large set of measurements of cathode and anode
            polarisations in a small-size cell with a reference electrode (three-electrode cell)
            and express the total polarisation  as a function of  local bulk gas composition,
            pressure, temperature, and current density. The essential condition is that the
            small-size cells (‘button cells’) use very little fuel gas and oxidant gas, so that the
            measured polarisation is representative for the bulk gas composition, pressure,
            and temperature at a given current level. The cell then functions as a differential
            reactor  that  provides  data  for  the  cell-  and  stack-level  (integral  reactor)
            modelling. Although small-size cell data are obviously useful and many such
            measurements are made. the effort implied in a full ‘polarisation mapping’ of this
            kind for each electrode is usually prohibitive. Moreover, the results are valid only
            €or the  range  over  which  the  operating  parameters  are  varied  and  for  the
            electrode-electrolyte  assembly microstructure  and configuration  used  in  the
            small-size cell.
              In lieu of an experimental ‘map’ of  polarisation, it is often desirable to have an
            electrode  model  that  provides  reliable  predictions  of  polarisation  of  either
            electrode over a wide range of operating and structural variables. This is the first
            purpose of the electrode model. But, conversely, to be a good predictor the model
            should be capable  of  interpreting  available polarisation  data for welI-defined
            conditions, that is, for small cells at low utilisation of  fuel or oxidant. Thus, the
            second purpose  of  an electrode model is to enable a more efficient process of
            collecting, correlating, and interpreting polarisation data. The electrode model
            is  capable  of  extracting the  kinetic  and  mass  transfer  (diffusion) resistance
            information  by  fitting  small-size  cell  polarisation  data.  It  provides  these
            resistance  characteristics  in  a  form  suitable  as  input  to  full-scale  cell  and
            stack models.
              An electrode model is especially advantageous if it can be used to relate the
            kinetic and mass transfer resistance to electrode geometry and microstructure:
            for instance, to thickness, porosity, pore or particle size, contact areas of  phases,
            and/or  grain  size  of  electrode  and  electrolyte  materials.  A  well-tested  and
            validated  electrode  model,  therefore.  may  serve  to  assist  in  the  design  of
            optimised electrode structures  or  electrode/electrolyte  interfaces  to  minimise
            polarisation loss.


            17.8.1 Fundamentals and Strategy of  Electrode-Level Models
            The objective of an electrode model is to analyse the point-to-point distribution of
            the reaction  in an SOFC electrode, leading  to current, potential, and species
            concentration  distributions. The result  of  the  analysis  is  a  prediction  of  the
            polarisation  of  the  electrode  due  to  (i) kinetic  resistance,  (ii) mass  transfer
            resistance, and (iii) ohmic resistance.
              The  analysis  includes  a  whole  set  of  material  properties  and  structural
            parameters. In principle it is based on the same fundamental laws used in full-
            scale cell analysis. Thus, mass transfer is subject to mass balances (Eqs. (1). (2)),
            heat flow to energy balances (Eqs. (5). (6)), and fluid flow to Eqs. (3), (4), but it
            is usually negligible in the pores of  the electrodes. In addition, current flow is
   338   339   340   341   342   343   344   345   346   347   348