Page 299 - High Temperature Solid Oxide Fuel Cells Fundamentals, Design and Applications
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2 76  High Temperature Solid Oxide Fuel Cells: Fundamentals, Design and Applications

          the  outlet  fuel  and  air  may  be  obtained  by  gas  analysis.  The  conversion
          resistance, Rp,,,n,,er may be calculated using the concept of Emf,,,:








            However, the anisotropic nature (temperature, gas composition, current flour)
          of a real cell under current flom7  often invalidates this  simple approach.  Gas
          conversion  under  electric load  causes an uneven  distribution of  the current
          density  with  decreasing  current  density  in  the  downstream  direction.  Fuel
          composition gradients over the cell originating from leaks cause different driving
          potentials at different points. In extreme cases, this may result in high Emf areas
          driving low Emf areas in electrolyser mode. Thus, internal currents may flow in
          the cell even at open circuit voltage (OCV). Gas leaks in the cell also affect the
          current  density  distribution  under  load  and  cause  localised  heating  by
          combustion. For tubular cell designs with high in-plane resistance, the current
          density distribution may be affected: furthermore, the temperature may not be
          constant  over  the  whole  cell  length  with  flowing  gases  adding  to  the
          inhomogeneity of the current density.
            Modelling can simplify or reduce the extent of  experimental task and predict
          likely behaviour under a broad range of  test conditions. However, subsequent
          validation by comparison with relevant cell and stack data is always important.
            An example of  the magnitude of  Rp,conver under different conditions can be
          deduced  from  Figure  10.10, which  shows  i-V  characteristics  obtained  in

                     0.7                                           1.1

                                                                   1
                     0.6
                                                                   0.9
                                                                      5
                                                                      Y
                   N
                   Z 0.5


                     0.4
                                                                   Ob
                                  ,
                     0.3                               8         I  0.4
                        0        0.2        0.4       0.6       0.8
                                    Current ctenslty  (Alcrn'}
          Figure  10.10  i-V  characteristics (right-hand scale) of  an anode-supported  cell tested in hydrogen with
          diflerent amounts of  water vapour in the fuel. Dashed lines are the ASRs as deduced from Eq. (l), and the solid
          lines are the cell resistances after correction for conversion of  the fuel, ASR,,,  (Eq. (3)). The cell temperature
          was850cCandthefuelJ?ou~was241/hinthecase with 5% H20and201/hforthe21%H~Ocase. Theairjow
                                   was 170 l/h. Cell area: 16 cm2.
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