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Cathodes  133

           interdiffusion of manganese, lanthanum and strontium ions across the interface
           into the YSZ  electrolyte. Tricker and Stobbs [48] confirmed, by examining the
           electrode/electrolyte  interface with  transmission  electron  microscopy  (TEM),
           that during high-temperature treatment, La2Zr207 is formed between LSM and
           YSZ, and that after 24 h the LazZr207 formed at the interface moves towards
           LSM,  leading  to  narrowing  of  the interface  with  the  YSZ.  The  latter  fact  is
           important in understanding the chemical nature of the La2Zr207 formation [49].
             To minimise reactions between the cathode and the electrolyte, in Japan, most
           research efforts have focused on the A-site-deficient lanthanum manganite. In
           the USA  and Europe, however, efforts [50] have been made to seek alternative
           cathodes, but with only limited success. Perhaps the most significant finding has
           been the use of composite cathodes in contact with the YSZ  electrolyte. These
           composite cathodes minimise cathode/electrolyte interaction by mixing LSM and
           YSZ powders and laying down a thin layer of this mixture on the electrolyte [lo].
           Another step forward has been the use of  an activation process to reduce the
           polarisation loss at the electrode [5 11.
             To  check  the  thermodynamic  predictions  of  the  cathode/electrolyte
           interaction,  effects of  the  A-site  deficiency in lanthanum manganite  on  the
           (cathode performance were investigated by Dokiya et al. [ 71 using the non-A-site-
           deficient and the A-site-deficient lanthanum manganites. It was found that the
           overpotential  is  smaller  when  the  A-site-deficient  lanthanum manganite  is
           applied at temperatures below  1473 K. Figure 5.10 shows a cell performance
           with the A-site-deficient lanthanum manganite cathode: the observed cathode
           overpotential (open circles) is compared with the evaluated resistivity (dashed
           line) originating from the electrolyte. The difference between two values gives
           the  overpotential from the cathode reaction, which is less than  30 mV  at a
           current density of 1400 mA cm-2.
             Yoshida et al. made systematic investigations on the effect of  using partially
           stabilised  zirconia  (PSZ, Y203  content  =  3  mol%) on  the  electrochemical
           performance of  cathodes with different dopants and their concentrations  [ 521.
           The overpotential of  the LSM/PSZ is always and systematically higher than that
           of the same LSM with fully stabilised YSZ. This is apparently due to the chemical
           interaction between LSM and PSZ; that is, the tetragonal phase (on the surface of
           the  PSZ  electrolyte)  is  transformed  into  the  cubic  phase  after  manganese
           dissolution into the tetragonal phase [5 31. This increases the overpotential of the
           LSM cathode.
             Although  the  A-site-deficient  LSM  can  avoid  reaction  with  YSZ,  its
           performance as cathode depends sensitively on its heat treatment temperature
           [7,54].  After  heat  treatments  at  lower  temperatures  below  1473 I<,  these
           cathodes exhibit excellent performance (see Figure 5.10, heat treated at 1423
           K), whereas heat treatment above this temperature gives rise to an increase in
           overpotential. Since no chemical reaction is expected as described above, this is
           due  to  the  diffusion  of  La  and  Mn  and  related  sintering  behaviour.  The
           sinterability  is enhanced in the A-site-deficient LSM.  It appears that diffusion
           inside  the  A-site-deficient  manganite  can  be  accelerated  by  increasing  the
           number  of  oxide ion  vacancies  at high  temperatures.  In addition, Zr  and Y
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