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Electrolytes  103

               Yokokawa et al. estimated  the electrolyte efficiency of  LSGM  used as the
           electrolyte in an SOFC [78]. Electrolyte efficiency was given by a function of fuel
           utilisation and internal resistance [ 761. When the thickness of the electrolyte was
           too small, chemical leakage of oxygen due to the electronic conduction became
           significant  and  the  extra  fuel  consumption  resulted  in decreased electrolyte
           efficiency. On the other hand, with increasing thickness of  electrolyte, internal
           resistance of  the cell increased also resulting in decreased electrolyte efficiency.
           Consequently, an optimum thickness exists for each electrolyte material at  a given
           temperature  and current density. For example YSZ operating at 700°C has an
           optimum thickness  of  about  10 pm. The benefit  of  LSGM  is  that its highest
           efficiency with a thickness near  5 pm is achieved around 450°C. Thus LSGM
           appears to be the best electrolyte discovered so far to operate at low temperatures.
             Several groups  have investigated  the electrochemical performance  of  cells
           with LSGM  electrolyte. Figure 4.22 shows the temperature dependence of  the
           maximum  power  density  and  the  open  circuit  voltage  (OCV)  of  a  cell with
           Smo.5Sro.5C003 cathode and Ni anode [79]. The OCV increased with decreasing
           temperature and was in good agreement with theoretical values estimated from
           the Nernst equation. The maximum power density was greater than 1.0 W/cm2
           at 1000°C and about 0.1 W/cm2 at 600°C with 0.5 mm thick LSGM electrolyte.
           in other  investigatfons  with LaGaQ3 based  electrolyte  [80-821  similar large
           power  densities  have  been  reported  at  intermediate  temperatures  with
          Lao~6Sro.4C003 cathode and Ni-CeOl doped with La cermet anode.

                          H,-3vol%H~O,Ni/Lao,~Sro~,Gao,~Mgo~~O~~Smo~~Sr~,~CoO~,
                                                           0,
                                                             1.5



















                                     Operating temperature /K
           Figure 4.22  Temperature dependence of the maximum power density nnd  the open circuit potential of the
                                   cell using LSGMfar electroIyte.


             Reactivity  of  LaGa03 with  electrode  materials  has  also  been  investigated
           [81,82]. Platinum seems to be easily reacted with gallium oxide to reduce Ga3+
           to Ga2+ which is volatile. As for the stability of  LaGa03-based electrolyte under
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