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. 2022 Aug 31;12(9):857. doi: 10.3390/membranes12090857
Generalities
Ji Molar flux of component i (gaseous species diffusing across the solid membrane)
Pi Permeability (coefficient) of component i (gaseous species diffusing across the solid membrane)
pi Partial pressure of component i in the gas mixture
fi Fugacity of component i in the gas mixture
l Membrane thickness
ci Penetrant molar concentration in the membrane phase
cu,i , cd,i Molar concentration (moles of gas/membrane volume) in the membrane phase on the upstream and downstream sides, respectively
Di Local diffusivity or diffusion coefficient of species i in the membrane
z Coordinate indicating the position along the membrane thickness
Li Mobility (or self-diffusion diffusivity) of species i in the membrane
μi Chemical potential of species i
Si Solubility coefficient of species i in the membrane Si=cipi
D¯i Concentration-averaged diffusivity of species i in the membrane
ωi Mass fraction of the fluid in the membrane
αi,j Selectivity of component i versus component j in the membrane
αi,jS Solubility-Selectivity of component i versus component j in the membrane
αi,jD Diffusivity-Selectivity of component i versus component j in the membrane
S0 Pre-exponential factor for solubility coefficient
ΔHs Heat of sorption
D0 Pre-exponential factor for diffusion coefficient
ED Activation energy of diffusion
P0 Pre-exponential factor for permeability coefficient
EP Activation energy of permeation
ΔHc Heat of condensation of the fluid species
ΔHm Heat of mixing of the fluid species in the membrane
Robeson’s upper bound
βi,j Gas couple-dependent parameter (position of the upper bound)
λi,j Gas couple-dependent parameter (slope of the upper bound)
dk,j Kinetic diameter of the larger molecule
dk,i Kinetic diameter of the smaller molecule
a Parameter used in the correlation for βi,j and λi,j
𝓫 Parameter used in the correlation for βi,j and λi,j
𝓯 Parameter used in the correlation for βi,j and λi,j
Activity coefficient models for solubility
γi Activity coefficient (of the fluid in the membrane)
ni Number of moles of component i in a mixture
Gex Excess Gibbs free energy of a mixture
G¯iex Partial molar excess Gibbs free energy for a component i in a mixture
LF EoS
G Gibbs free energy
N Total number of molecules
kB Boltzmann’s constant
nc Number of components (gases + polymer)
Mi Molar mass of component i
ρi Density of component i
vi* Molar volume of a lattice cell of component i
ri0 Number of lattice cells occupied by a molecule of pure component i
εi Non-bonded interaction energy between two lattice cells occupied by component i
Ti* Characteristic temperature of component iTi*=εikb
pi* Characteristic pressure of component ipi*=εivi*
ρi* Characteristic density of component iρi*=Mirivi*
T˜i Reduced temperature of component iT˜i=TTi*
p˜i Reduced pressure of component ip˜i=ppi*
ρ˜i Reduced density of component iρ˜i=ρiρi*
ρ Density of the mixture
T˜ Reduced temperature T˜=T/T*
p˜ Reduced pressure p˜=p/p*
ρ˜ Reduced density ρ˜=ρ/ρ*
kij Binary interaction parameter between i and j
ωi Mass fraction of component i
ϕi Volume fraction of component i in close-packed conditions ϕi=ωi/ρi*iNωi/ρi*
ρ* Characteristic density of the mixture 1ρ*=incωiρi*
p* Characteristic pressure of the mixture
p*=incϕipi*inc1j>incϕiϕjΔpij*
pij*=pi*+pj*2(1kij)pi*·pj*
T* Characteristic temperature of the mixture T*=p*iNpi*ϕiTi*
v* Average close-packed molar volume in the mixture v*=T*Rp*
ri Number of lattice cells occupied by a molecule in mixture ri=ri0vi*v*
NRHB EoS
εi* Characteristic energy in the LF model and in the NRHB model
εi,h* Enthalpic contribution to the characteristic energy
εi,s* Entropic contribution to the characteristic energy
Eαβ0 Association energy between group α and a functional group β
Sαβ0 Association entropy between a functional group α and a functional group β
SAFT EoS
Ares Residual Helmholtz free energy (at fixed temperature and volume)
Ahs Hard-sphere term of residual Helmholtz free energy
Adisp Dispersion term of residual Helmholtz free energy
Achain Chain term of residual Helmholtz free energy
Aassoc Association term of residual Helmholtz free energy
μiIG Chemical potential of species i in the ideal gas state
NET-GP model for solubility
μiNE Non-equilibrium chemical potential of species i
μiEq Equilibrium chemical potential of species i
ρpol Non-equilibrium density of the glassy polymer
μiNE(pol) Non-equilibrium chemical potential of species i in the polymer phase
μiEq(gas) Equilibrium chemical potential of species i in the gas phase
ω¯ Composition vector in the polymer phase
y¯ Composition vector in the gas phase
ρpol0 Non-equilibrium density of the dry glassy polymer
ksw,i Swelling coefficient correlating the glassy polymer density to the gas i partial pressure
DMS model for solubility
kD,i Henry’s law constant
CH,i Langmuir capacity constant
bi Langmuir affinity constant
kD0 Pre-exponential factor for temperature-dependence of kD
b0 Pre-exponential factor for temperature-dependence of b
HD Enthalpy of sorption for Henry’s mode of sorption
Hb Enthalpy of sorption for Langmuir’s mode of sorption
GAB model for solubility
v Penetrant adsorbed mass ratio
p Adsorbate pressure
p* Reference pressure value associated with the adsorbate
vm Capacity of the 1st adsorption monolayer
h Dimensionless binding parameter
rij Parameter related to sorbate–sorbate interactions in multicomponent GAB
hij Parameter related to sorbate–sorbate interactions in multicomponent GAB
Fractal model for solubility coefficient
Fgef Effective cross-sectional area of the sorbed gas molecules
Df Global fractal dimension parameter
S0 Minimum solubility of a gas molecule
φcl Relative fraction of the closely packed segments in clusters
Tg Polymer glass transition temperature
Xcr Degree of crystallinity
df Fractal dimension of the polymer structure
Acr Cross-sectional area of a macromolecule
CS Characteristic ratio representing the index of chain flexibility
Free-volume theory for diffusion coefficient
D1,self Self-diffusion coefficient of fluid 1 in polymer 2
D10 Pre-exponential factor = diffusion in a fluid with infinite free volume
ED0 Energy required for a jump into an adjacent free-volume void
γ Coefficient accounting for overlaps of free volume available to adjacent molecules
Vi* Occupied volume
VF Average free volume per jumping unit
ξV1*V2* Ratio of occupied volumes
K1i,K2i Parameters for component i related to pure component viscosity
α1 Thermodynamic factor of mutual diffusivity
FFV Fractional free volume
A,B Adjustable parameters for correlation between diffusivity and FFV
Vpol Polymer-specific volume
Vpol* Polymer-occupied volume
Fractal model for diffusion coefficient
D0 Universal constant of the model, equal to 3.8 × 10−7 cm2/s
fg Relative free volume
dh Diameter of a microvoid
dm Diameter of the penetrant gas molecule
ds Polymer chain spectral dimension
Maxwell–Stefan model for diffusion coefficient
Đ Maxwell–Stefan diffusivity
vAvB Velocity of species A relative to species B
Γ Thermodynamic correction factor
Ni Total molar flux of species i (with respect to a fixed reference frame)
𝓃t Total molar concentration of the fluid mixture
xi Mole fraction of component i in the mixture
Partial Immobilization Dual-Mobility Model for Permeability
Ni Total molar flux of component i
CD,i Penetrant concentrations in the Henry’s region
CH,i Penetrant concentration in the Langmuir’s region
DD,i Diffusivity in the Henry region
DH,i Diffusivity in the Langmuir region
Fi Ratio between diffusivity in Henry’s region and Langmuir’s regions
Ki Ratio between Dual-Sorption Mode Model parameters
pu,i Upstream partial pressure of component i
pd,i Downstream partial pressure of component i
Standard Transport Model for Permeability
Li Mobility coefficient of component i
Li,0 Infinite dilution mobility coefficient of component i
β Plasticization factor
Mi Penetrant molecular weight
Zi Penetrant compressibility factor
ρpol Polymer density
ϱ Size selectivity of the polymer
τ Polymer-dependent parameter in the empirical correlation between penetrant mobility and critical volume
ϱ0 Pre-exponential factor for parameter η
Vc Critical volume of penetrant
Widom insertion method
μiex Excess chemical potential of penetrant i inside the polymer
ΔUtestinter Potential energy of interaction between the test molecule and the other molecules
Simulation of diffusivity
(ri(t)ri(0))2 Mean squared displacement (MSD) averaged over all molecules
t Time
Di,selfMD Self-diffusion coefficient computed in the MD simulations
η Shear viscosity computed in MD simulations
Ξ Dimensionless constant equal to 2.837298 for periodic (cubic) lattices
Λ Simulation box length