2.5 Measurement of liquid-phase diffusion coefficient
There are few methods of determination of liquid-phase diffusivities. The most commonly used method is Diaphragm cell method.
2.5.1 Diaphragm cell method
Diaphragm cell contains two compartments as shown in Figure 2.8. These are separated by diaphragm. Let the area of the diaphragm is ‘a’ and porosity is ‘ε’. Effective area for diffusion = a ε
(2.49)
where τ is tortuosity. As the solute concentration is very low, bulk flow term can be taken as zero. Hence,
Figure 2.8: Diaphragm cell
(2.50)
(2.51)
and (2.52)
Adding Equations (2.51) and (2.52) and substituting NA from Equation (2.50) we have,
(2.53)
Boundary conditions
Therefore, (2.54)
2.5.2 Semi-empirical Equation: Wilke-Chang Equation
(2.55)
where, D0AB is diffusivity of solute A in solvent B, m2/s, φ is association factor [for H2O=2.26; MeOH=1.9; EtOH=1.5; non-associated solvent=1.0]; MB is molecular weight of B; T is absolute temperature in K; μB is solution viscosity, kg/m.s; νA is solute molar volume at normal boiling point, m3 /kmol [νA=0.0756 m3/kmol for H2O as solvent].
2.5.3 Stokes-Einstein Equation
Liquid diffusivity varies linearly with absolute temperature and inversely proportional to viscosity of the medium. Hence,
(2.56)
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