Page 323 - High Temperature Solid Oxide Fuel Cells Fundamentals, Design and Applications
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Cell. Stack and System Modelling  299

           element and depending on the mismatch in coefficients of  thermal expansion
           between  cell components. The configuration of  the manifolds and overall cell
           dimensions can be modified based on the thermal stress results. The simulation
           can also be used to optimise the stack geometry for flow uniformity.



           '111.3 Continuum-Level Electrochemistry Model
           One of  the most important  aspects of  SOFC design is the voltage  and current
           distribution in the PEN. This couples with the temperature distribution from the
           flow model and also with the electrochemical reactions at the electrodes. The
           electrochemical process generates electrical power and heat, but excessive heat
           generation  must  be  avoided since it may  cause thermal stresses affecting the
           structural stability of the SOFC.
             At the effective property or continuum level, the simulation of electrode and
           cell performance basically requires only a parameterised electrochemical model.
           Such  an  electrochemical  model  is  usually  described  as  a  current-voltage
           relation, or I-V  curve, for a single cell, in terms of parameters that are effective
           cell  properties  and  operational  parameters.  The  I-V  relation  describes  the
           voltage  (potential)  loss  at  a  specified  current  with  respect  to  the  ideal
           thermodynamic performance, which is called overpotential or polarisation (q).
           This cell I-V  curve is specific for the materials, structural characteristics, and
           operational parameters  (gas compositions, pressure, temperature) of  a given
           PEN element.
             As an analogy to mass and energy balances, one can write a potential balance
           of the fuel cell as follows [lo]:

               v(i) = Eeq  - iRi - Vc - VA  = Eeq - iRi - VCa  - VCc - VAa  - VAc   (7)

           Here E,,  is the equilibrium (open circuit) voltage, or emf (electromotive force) of
           the cell, i is the current density, iRi is the ohmic potential drop, and qc and qA
           are the polarisation  of  the  cathode  and the  anode,  respectively.  As  shown
           in  Eq.  (7) each  of  the  polarisation  may  be  further  split  in  an  activation-
           related  contribution (subscript a) and a concentration  (i.e., diffusion) related
           contribution (subscript c).
             The  thermodynamic  cell  potential,  Eeq, depends  on  reactant  and  product
           partial pressures as well as temperature. For example, for the hydrogen/oxygen
           fuel cell






           where R is the gas constant, T is the temperature, and F is the Faraday constant.
           AG" is the standard free-energy change of the reaction Hz + 1/202  --f  H20; Le.,
           the  free-energy  change  when  reacting  species  and  products  are  all  at  the
           standard pressure of  1 atm. The first term on the right-hand  side of  Eq.  (gat,
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