Page 174 - High Temperature Solid Oxide Fuel Cells Fundamentals, Design and Applications
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Anodes  151

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         Figure  6.1  Schematic  of  anode  cermet  structure,  showing  interpenetrating  networks  of  pores  and
         conductors - nickrl for electrons, yttria-stabilised  zirconia for oxide ions. The reactive sites are the contact
                zonesofthe twoconductingphases whichareaccessible to fuel through theporosityr21.
         discharge electrons to the conducting anode. This requires gas phase for the fuel
         access, electrolyte phase for oxide ion entry and metal phase for electron output,
         the so-called ‘three-phase boundary’ zone. For efficient operation this should not
         be simply a linear structure at a two-dimensional interface of the solid materials,
         but rather distributed to provide an active ‘volumetric’ reaction region in three
         dimensions.  Consequently,  the  fabrication  of  the  anode  is  important  in
         determining this complicated three-phase structure.



         6.3  Choice of  Cermet Anode Components

         Given  these  stringent  requirements,  only  a  few metallic  or  ceramic  candidate
         materials are available. After the ‘Nernst mass’, now known as yttria-stabilised
         zirconia had been identified as the favoured high-temperature ceramic electrolyte,
         Baur and Preis evaluated iron and graphite as anode materials [3]. Graphite, of
         course, is susceptible to electrochemical oxidative corrosion, so that cell life with
         a graphite  anode is unduly short. Platinum also attracted  attention due to its
         high-temperature stability and catalytic properties, as did other transition metals
         as presented in the historical review by Mobius [4]. Even platinum, however, was
         unsuccessful as its bond to the electrolyte tends to fail in service, with the anode
         layer spalling off probably due to electrochemical generation of water vapour at
         the  interface.  The transition  metals  also  have  limitations.  Iron  is  no  longer
         protected  by  the reducing activity of  the fuel gas once the partial pressure  of
         oxidation  products  in the anode compartment exceeds a critical value, and it
         then corrodes with formation of a red iron oxide. Cobalt is somewhat more stable,
         but  also more costly. Nickel has a significant thermal expansion  mismatch to
         stabilised  zirconia,  and  at high  temperatures the metal  aggregates  by  grain
         growth,  finally  obstructing  the  porosity  of  the  anode  and  eliminating  the
         three-phase boundaries required for cell operation. As a consequence, all-metal
         anodes  have not  found  acceptance  in SOFC  technology.  Pure ceramic  oxide
         anode technology is a very recent development and is discussed later.
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