Abstract

The deposition of several alternating anion- and cation-exchange surface layers (layer-by-layer method) is a promising technique for the modification of ion-exchange membranes, which makes it possible to essentially increase their selectivity to singly charged ions. This paper presents a one-dimensional model, which is based on the Nernst–Planck–Poisson equations and describes the competitive transfer of singly and doubly charged ions through a multilayer composite ion-exchange membrane. It has been revealed for the first time that, as in the earlier studied case of a bilayer membrane, the dependence of the specific permselectivity coefficient (P1/2) of a multilayer membrane on the electrical current density passes through a maximum left( {P_{{{1 mathord{left/ {vphantom {1 2}} right. kern-0em} 2}}}^{{max }}} right). It has been shown that an increase in the number of nanosized modification bilayers n leads to the growth of P_{{{1 mathord{left/ {vphantom {1 2}} right. kern-0em} 2}}}^{{max }}, but the flux of a preferably transferred ion decreases in this case. It has been established that P_{{{1 mathord{left/ {vphantom {1 2}} right. kern-0em} 2}}}^{{max }} is attained at underlimiting current densities and relatively low potential drop. The simulated dependences P_{{{1 mathord{left/ {vphantom {1 2}} right. kern-0em} 2}}}^{{max }}(n) qualitatively agree with the known literature experimental and theoretical results.

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