Page 104 - Introduction to Transfer Phenomena in PEM Fuel Cells
P. 104

Mass Transfer Phenomena     93
                             Darcy’s law, which describes the convection of a gas mixture in a porous
                           medium (diffusion layers), is based on the homogenization of porous and
                           fluid media in a place where the detailed geometric description of the pore
                           structure is not necessary [GAL 05]. In this case, the volume of the medium
                           is considered relatively large in relation to the pore size; therefore, the speed
                           of the gas mixture is determined by the pressure gradient, the viscosity and
                           the structure of the porous medium [NGU 10]:
                                     k    
                                 u =−  P  ∇ p                                            [3.17]
                                      μ

                           where:

                                                                        –1
                                                                     –1
                             – µ is the dynamic viscosity of the gas [kg.m .s ];
                             – K p is the permeability [m²];
                             – P is the pressure [Pa].


                           3.4.2. The conservation of species

                             The species conservation equation representing conservation of mass for
                           the gas phase of a single species is written as [BAR 05]:

                                                                      
                                             
                                                        
                                  ( ∂ρ⋅ε⋅ w i )  +∇ ( ρ⋅ε⋅ wu = ∇ ρ⋅ D eff  ⋅∇ w + S     [3.18]
                                                            
                                                         ) (
                                                       ⋅
                                      t ∂             i           i       ) i  s,i
                           where:
                             –  w  is the mass fraction of the species (i) in its gaseous phase (H 2, O 2,
                                 i
                           H 2O and N 2);
                             – S s,i is the source term (or well) of the species (i);

                             –  D eff   is the diffusion coefficient of the species (i) in a porous
                                 i
                                             –1
                           environment in [m².s ];
                                 ( ∂ρ⋅ε⋅ w  )
                             –          i   is the species accumulation term;
                                     t ∂
                                        
                             –  ( ρ⋅ε⋅ wu  )  is the advection term;
                               ∇
                                         ⋅
                                        i
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