Page 109 - Introduction to Transfer Phenomena in PEM Fuel Cells
P. 109

98     Introduction to Transfer Phenomena in PEM Fuel Cells
                             – at the cathode:
                               - the gas mixture is ternary, the species involved are oxygen, nitrogen
                           and water vapor; the equation system to solve is written as:
                           
                           
                                      c
                            x O 2  +  x N 2  +  x  = 1
                                      HO
                                       2
                                            N c   
                            dx N  1   N O    H O 
                              2  =⋅    2  +    2    x ⋅  N                            [3.32]
                             dx  c    D eff  D eff    2
                                     O,N 2  H O,N 2 
                                               2
                                        2
                                         c                                         
                            dx O  1   N O 2  +  N H O    1    1              N O   
                              2  =⋅    eff  2  x ⋅  O 2  +   eff  −  eff    ⋅  N O 2  x ⋅  N 2  −  eff  2  
                             dx  c    D             D      D                D O,H O 
                                       O,H O          O,H O  O,N 2            2  2 
                                                        2
                                                                 2
                                                          2
                                           2
                                         2
                               - at the diffuser inlet, the relative humidities (RH) are  expressed as
                           follows:
                                            p
                                  x ce  =  HR ⋅  sat
                                           c
                                    2
                                   HO        p
                                                  p  
                                              −
                                  x e O 2  = 0,21 1 HR ⋅  sat                         [3.33]
                                           
                                                  c
                                                      p
                                            
                                                   p   
                                  x e  =  0,79 1 HR ⋅  sat  
                                              −
                                            
                                   N 2          c  p  
                           3.4.3. Some parametric laws
                           3.4.3.1. Saturation pressure
                             Different formulas have  been proposed for determining the saturation
                           pressure of  water (in  [Pa]). Wöhr presented, in his work, the following
                           empirical formula [MON 06]:
                                              A−  B    
                                 P sat  () 10=    C T 273   +−  ⋅ 100                  [3.34]
                                     T
                             In this relation, the temperature is in Kelvin, and the coefficients have the
                           following values: A = 8.073; B = 1 656.39; C = 226.86 in K. Chun-Ying
                           Hsu et al. [WÖH 00] used another formula where the decimal logarithm of
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