Abstract
Heterogeneous catalysis is of paramount importance in many areas of gas conversion and processing in chemical engineering industries. In porous pellets, the catalytic reactions may be affected by diffusional limitations such that the global rate can be different from the intrinsic reaction rate. In the literature, a number of multicomponent diffusion flux closures have been applied to characterize the diffusion process within different units in chemical process plants. The main purpose of this paper is to outline the derivation of the different diffusion flux models: the rigorous Maxwell–Stefan and dusty gas models, and the simpler Wilke and Wilke–Bosanquet models. Usually the diffusion fluxes are derived and presented with respect to the molar average velocity definition. In this study, also the diffusion flux closures with respect to the mass average velocity definition is outlined. Thus, if the temperature equation and the momentum equation are used in the pellet model, a consistently closed set of pellet equations is obtained on mass basis holding only the mass average velocity. On the other hand, for the closed set of pellet equations on molar basis, the component balances hold the molar averaged velocity whereas the temperature and momentum equations hold the mass average velocity due to the physical laws applied deriving these fundamental balances. Nevertheless, the Maxwell–Stefan and dusty gas models are manipulated and put on the convenient Fickian form. The second purpose of this article is the evaluation of the diffusion flux closures derived. For this purpose, a transient model is developed to describe the evolution of the species composition, pressure, velocity, temperature, total concentration, and fluxes within a spherical pellet. The catalyst problem has been simulated for the methanol dehydration process producing dimethyl ether (DME), with computed efficiency factor values in the range 0.06–0.6 for pellet pore diameters of 0.1–100 nm. Identical results are expected for the mole and mass based pellet equations. However, deviations are obtained in the component fractions comparing the mass and mole based pellet model formulations where the mass fluxes were described according to the Wilke and Wilke–Bosanquet models. On the other hand, the rigorous Maxwell–Stefan and dusty gas models gave identical results.
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Abbreviations
- B :
-
Permeability, m2
- c :
-
Concentration, kmol/m3
- Cp :
-
Heat capacity, J/(kmol K)
- Cp′′:
-
Heat capacity, J/(kg K)
- D :
-
Diffusivity, m2/s
- \({\widetilde D_{ij}}\) :
-
Maxwell–Stefan diffusivities, m2/s
- D ij :
-
Binary diffusion coefficient for species i and j, m2/s
- D im :
-
Diffusion coefficient of species i in Wilke molar flux, m2/s
- \({D_{i{\rm m}}^{''}}\) :
-
Diffusion coefficient of species i in Wilke mass flux, m2/s
- D iK :
-
Knudsen diffusion coefficient for species i, m2/s
- D i,eff :
-
Bosanquet diffusivity, mole basis, m2/s
- \({D''_{i,{\rm eff}}}\) :
-
Bosanquet diffusivity, mass basis, m2/s
- d i :
-
Diffusional driving force, m−1
- d p :
-
Diameter of pellet, m
- d pore :
-
Average pore diameter, m
- g :
-
External force per unit mass, m/s2
- h :
-
Heat transfer coefficient, W/(m2K)
- ΔH :
-
Heat of reaction, J/kmol
- J :
-
Molecular diffusion flux, kmol/(s m2)
- j :
-
Mass diffusion flux, kg/(s m2)
- k :
-
Reaction rate constant, kmol/(kg h)
- k :
-
Boltzmann constant, 1.3805 · 10−23, J/K
- k :
-
Mass transfer coefficient, m/s
- K M, K W :
-
Adsorption constant, m3/kmol
- K :
-
Thermodynamic equilibrium constant, dimensionless
- M :
-
Molecular weight, kg/kmol
- N :
-
Number of collocation points, dimensionless
- n :
-
Number of species in gas mixture, dimensionless
- n i :
-
Combined mass flux of species i in gas mixture, kg/(m2s)
- N i :
-
Combined molar flux of species i in gas mixture, kmol/(m2s)
- p :
-
Pressure, Pa
- Q :
-
Heat conductivity flux, J/(m2s)
- R :
-
Gas constant, J/(kmol K)
- r :
-
Radial coordinate, m
- r :
-
Reaction rate, kmol/(kg s)
- r M :
-
Reaction rate, kmol/(kg h)
- r p :
-
Radius of pellet, m
- S :
-
Molecular source term, (kmol)/(m3s)
- S′′:
-
Mass source term, kg/(m3s)
- Ŝ :
-
Heat source term, J/(m3s)
- T :
-
Temperature, K
- t :
-
Time, s
- u :
-
Molar average velocity, m/s
- v :
-
Mass average velocity, m/s
- v i :
-
Velocity of species i with respect to fixed coordinates, m/s
- V :
-
Volume, m3
- x :
-
Mole fraction, dimensionless
- η :
-
Effectiveness factor, dimensionless
- \({\epsilon}\) :
-
Porosity, dimensionless
- \({\epsilon}\) :
-
Characteristic Lennar-Jones energy, J
- λ :
-
Conductivity, W/(m K)
- ρ :
-
Density, kg/m3
- τ :
-
Tortuosity, dimensionless
- μ :
-
Dynamic viscosity, kg/(m s)
- ω :
-
Mass fraction, dimensionless
- Ω :
-
Diffusion collision integral, dimensionless
- Σ :
-
Characteristic Lennard-Jones length, Å
- b:
-
Bulk
- i, j, n :
-
Species type
- M:
-
Methanol
- p:
-
Pellet
- r :
-
Radial direction
- ref:
-
Reference state
- W:
-
Water
- *:
-
Dimensionless variable
- ′:
-
Gas mixture with dust particles
- ′′:
-
Mass basis
- ′′:
-
Second-order derivative in finite difference scheme (69)
- b:
-
Bulk
- e:
-
Effective
- s:
-
Superficial
- s:
-
Pellet surface; equation (71)
- τ :
-
Time level
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Solsvik, J., Jakobsen, H.A. A Survey of Multicomponent Mass Diffusion Flux Closures for Porous Pellets: Mass and Molar Forms. Transp Porous Med 93, 99–126 (2012). https://doi.org/10.1007/s11242-012-9946-7
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DOI: https://doi.org/10.1007/s11242-012-9946-7