The Maxwell–Stefan diffusion (or Stefan–Maxwell diffusion) is a model for describing diffusion in multicomponent systems. The equations that describe these transport processes have been developed independently and in parallel by James Clerk Maxwell for dilute gases and Josef Stefan for liquids. The Maxwell–Stefan equation is
a i ∇ μ i R T = ∇ a i = ∑ j = 1 j ≠ i n χ j D i j ( v → j − v → i ) = ∑ j = 1 j ≠ i n c j c D i j ( J → j c j − J → i c i ) {\displaystyle a_{i}{\frac {\nabla \mu _{i}}{R\,T}}=\nabla a_{i}=\sum _{j=1 \atop j\neq i}^{n}{{\frac {\chi _{j}}{{\mathfrak {D}}_{ij}}}({\vec {v}}_{j}-{\vec {v}}_{i})}=\sum _{j=1 \atop j\neq i}^{n}{{\frac {c_{j}}{c{\mathfrak {D}}_{ij}}}\left({\frac {{\vec {J}}_{j}}{c_{j}}}-{\frac {{\vec {J}}_{i}}{c_{i}}}\right)}}
∇: vector differential operator χ: Mole fraction μ: Chemical potential a: Activity i, j: Indexes for component i and j n: Number of components
D i j {\displaystyle {\mathfrak {D}}_{ij}} : Maxwell–Stefan-diffusion coefficient
v → i {\displaystyle {\vec {v}}_{i}} : Diffusion velocity of component i
c i {\displaystyle c_{i}} : Molar concentration of component i c: Total molar concentration
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