Page 85 - High Temperature Solid Oxide Fuel Cells Fundamentals, Design and Applications
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62  High Temperature Solid Oxide Fuel Cells: Fundamentals, Design and Applications

         cumulative volume of the reactants. But the cumulative volume of the reactants
         and of the products of the oxidation reaction of methane is the same. This is also
         apparent by the values of the activity K (In( 1) = 0). Thus there is theoretically no
         change of the entropy in the last case and the real change of the measured values
         at the standard state 0 is very limited as indicated in Table 3.1. This is the reason
         for  the  very  small  dependence  on  temperature  of  the  free  enthalpy  or  the
         reversible  cell  voltage  of  the  oxidation  reaction  of  methane,  the  idealised
         pressure dependence of the entropy yields no change in the cell voltage caused by
         the system pressure. The reversible cell voltage of the hydrogen and the carbon
         monoxide  oxidation  decreases  with  increasing  system  temperature  and
         increases with increasing system pressure.



         3.3.  Voltage losses by Ohmic Resistance and by Mixing Effects by
         Fuel  Utilisation
         The  thermodynamic  relevance  of  the  voltage  can  be  understood  by
         considering Eqs. (13) and (16). The voltage is a measure of the exergetic quality
         similar to the work of  a thermodynamic process. The exergy is defined as the
         potential of the reversible work of  a system related to the ambient state 0 [l].
         Thus  it  is  clear  that  the  voltage  loss  AV due  to  the  electric resistance  R  is
         connected with  an additional irreversible production  of  entropy.  We  get  for
         the voltage loss

             AV=I*R                                                        (30)
         and for the power loss

             Pioss = AV +  I = I2 . R = Tsopc . Uf . ~FI Asirr.            (31)
                                              *
           Equation (3 1) shows that the irreversible entropy production of an ohmic loss
         Ploss in  a SOFC is  smaller than that in another fuel cell operating at a lower
         temperature  and a generalised form of Eq. (13) yields the irreversible entropy
         production





           Equation (1 3) was generalised here as

             I = -ne'  . Uf . hFI . E.                                     (33)

           It has already been mentioned that the mixing effects during fuel utilisation
         within a SOFC do not allow a reversible SOFC operation. These influences and the
         voltage  reduction can be  easily calculated by  considering  the fuel utilisation
         connected with a change of  the partial pressures of  the components within the
         system [2].
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