Abstract
The ideal case of an ion-exchange resin is that of a homogeneous isotropically-swelling gel with a regular distribution of charged functional groups throughout the particle. For convenience, the particle geometry should be spherical, since this requires only one parameter for its definition, and of course each particle should have the same radius. The charged groups should each have a single counterion, and the Donnan membrane effect should permit virtually no invasion of external electrolyte. When considering the exchange of ions in such a system, both the original counterion and the ion for which it exchanges should be of the same size, hydration, and valency, and should have identical diffusion coefficients both in the external solution, and inside the homogeneous gel phase. Again for convenience we should wish the resin to show no preference for one ion rather than the other.
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© 1983 Martinus Nijhoff Publishers, The Hague
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Millar, J.R. (1983). On the Structure of Ion-Exchange Resins. In: Liberti, L., Helfferich, F.G. (eds) Mass Transfer and Kinetics of Ion Exchange. NATO ASI Series, vol 71. Springer, Dordrecht. https://doi.org/10.1007/978-94-009-6899-8_2
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DOI: https://doi.org/10.1007/978-94-009-6899-8_2
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