Page 200 - High Temperature Solid Oxide Fuel Cells Fundamentals, Design and Applications
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Interconnects  177

           conductivity and can survive such reducing conditions. Thus, the chromites are
           quite unique  and are the only oxides available for use as interconnects. The
           LaCr03 doped with either Ca or Sr has sufficient conductivity in fuel atmospheres
           to exceed 1 S/cm and therefore is preferred to Mg-doped LaCr03.
             There  has  been  some  concern  about  the  oxygen  ion  conductivity  in
           (La,SrCa)Cr03,  particularly  under  reducing  conditions,  but  studies  by
           Yokokawa  et  al.  [9]  and  Singhal  [lo] suggest  that  this  is  not  a  serious
           problem since at 1000°C the oxygen diffusion coefficient appears to be less than
                cm2/s. This would yield an ionic transport number of less than 0.01 even at
           the  most  reducing  conditions.  Thus,  oxygen  permeation  through  the
           interconnect should be minimal.


           7.2.2 Thermal Expansion
           It is important that the thermal expansion coefficients of  all SOFC components
           match well. This is particularly true for the dense components, the electrolyte
           (most commonly yttria-stabilised zirconia, YSZ) and the interconnect. Table 7.3
           compares the thermal expansion coefficients (TECs) and shows that the TECs of
           LaCr03 and YCr03 do not match that of  YSZ, but the addition of  dopants makes
           the  match  possible.  Thus,  thermal  expansion  is  not  a  significant  problem.
           However, the loss of  oxygen in a reducing atmosphere leads to lattice expansion
           which has the potential of  causing cracking problems [lo-181. For example, at
           1000°C, when  exposed  to  hydrogen,  LaCro.8&go.l 503  and  Lao.8Sro.2Cr03
           expand  about  0.1% and  0.3%,  respectively  (Figure  7.4).  The  amount  of
           expansion  due  to  oxygen  loss  is  directly  related  to  the  oxygen  vacancy
           concentration. Several studies have shown that this expansion can be minimised
           by the addition of elements such as A1 and Ti, but it is difficult to completely avoid
           this  behaviour  without  the  loss  of  other  desirable  properties,  such  as  the
           electrical conductivity [16, 181. Thus, it is important to allow for this expansion
           in the cell and stack design.




           Table 7.3  Thermal expansion coefficients of LaCrO:, andYCr03 p-131
           Composition (nominal)                           Thermal expansion coefficient
                                                            (x 10-6/K)
           LaCr03                                           9.5
           LaCro.gMg0.103                                   9.5
           Lao.gSro.lCr03                                   10.7
           Ladr0.2CrO3                                      11.1
           h~Cao.3 003                                      10.8
           La%.&o0.103                                      13.1
           La0.8Ca0.2Cro.sCoo.lO3                           11.1
           YCr03                                             7.8
           Yo.YC~O.IC~O~                                     8.9
           Yo.sC~O,~C~O~                                     9.6
           YSZ                                               9.4-11
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