Page 518 - Advanced thermodynamics for engineers
P. 518

21.2 THEORY OF FUEL CELLS        511




                  Equations (21.32) and (21.34) show quite distinctly that the processes taking place in the fuel
               cell are governed by similar equations to those describing combustion. The equations are similar to
               those for dissociation, which also obeys the Law of Mass Action. In the case of gaseous components
               the activity can be related to the partial pressures by a i ¼ p i /p 0 ,where p i ¼ partial pressure of
               component i.
               21.2.3.1 Example: a hydrogen–oxygen fuel cell
               Consider a fuel cell in which the fuel is hydrogen and oxygen, and these gases are supplied down the
               electrodes. A suitable electrolyte for this cell is aqueous potassium hydroxide (KOH). The cell can be
               defined as

                                                 H 2 jKOHðaqÞjO 2                          (21.35)
                  The basic reactions taking place at the electrodes are
                                       H 2 þ 2OH /2H 2 O þ 2e  at hydrogen electrode

                                                                                           (21.36)
                                  1
                                    O 2 þ H 2 O þ 2e/2OH      at oxygen electrode
                                  2
               and these can be combined to give the overall reaction

                                             1
                                        H 2 þ O 2 /H 2 O                                   (21.37)
                                             2
                  It can be seen that the KOH does not take part in the reaction, and simply acts as a medium through
               which the charges can flow. It is apparent from Eqn (21.36) that the valency (z i ) of hydrogen is 2. From
               Eqn (21.34), the cell open circuit potential, the standard emf, is given by

                        DG 0      ½ 30434:3   0:5   52477:3  ð 239081:7   46370:1ފ
                   0       298
                  E ¼         ¼                                                 ¼ 1:185 V  (21.38)
                           F                        2   96485
                        z H 2
                  The standard emf in Eqn (21.38) has been evaluated by assuming that the partial pressures of the
               gases are all 1 atm. In an actual cell at equilibrium they will be controlled by the chemical equation,
               and the actual emf achievable will be given by an equation similar to Eqn (21.34) which includes the
               partial pressures of the constituents, viz

                                               0 Q      n  1           0 Q     n  1
                                                       p r                    p r
                                   DG  0 T  <T  B products    0  <T    B products
                                                         C
                               E ¼           ln @ Q      A ¼ E      ln @ Q      C          (21.39)
                                    z i F  z i F       p v r      z i F       p n r  A
                                                 reactants              reactants
                  Equation (21.39) can be written in a shorter form as
                                        DG 0 T  <T    Y       0  <T      Y
                                                        n
                                                                           n
                                   E ¼            ln   p r  ¼ E     ln    p r             (21.39a)
                                        z i F  z i F              z i F
               where the stoichiometric coefficients, n, are defined as positive for products and negative for reactants.
   513   514   515   516   517   518   519   520   521   522   523