4.6 Article

Low-frequency impedance of an ion-exchange membrane system

Journal

ELECTROCHIMICA ACTA
Volume 53, Issue 22, Pages 6380-6390

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.electacta.2008.04.041

Keywords

ion-exchange membrane; diffusion boundary layer; impedance; mathematical modelling; concentration polarization

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A I D mathematical description of low-frequency impedance is presented for a system including an ionexchange membrane, two adjacent diffusion boundary layers (DBLs) and two layers of bulk solution. Electrolyte concentration may vary within the DBLs under the action of a direct current (DQ and a small sinusoidal current perturbation imposed on the DC. The description is based on the Nernst-Planck equations and the local electroneutrality assumption, which are believed correct at current densities lower than the limiting one. The results of calculations are compared with experimental data obtained for an AMX anion-exchange membrane installed in a cell with a well specified forced laminar flow of a 0.02 M NaCl solution. For each applied DC density, two fitting parameters, the DBL thickness and the ohmic resistance of the membrane and two bulk solution layers are found. It is shown that the experimental spectra are well described by the model. The hyperbolic tangent element, tanh cilce, acts an important role in the impedance behavior of membrane system, similar as in electrode systems with an open diffusion layer of a finite thickness, or 0 element, which provides a finite thickness porous Warburg impedance. The relevant parameter found by fitting the experimental data is the thickness of depleted DBL, which increases slightly with increasing DC density, but remains close to Nernst's DBL thickness calculated by using the 21) convective-diffusion model. It is found that the main contributions to the impedance are the Dorman contribution, which is due to the variation of interfacial potential drops caused by boundary concentration variations, and the conductivity contribution becoming important at high currents. The last contribution, first considered in this paper, is due to the variation of the solution conductivity resulting from the concentration variation caused by an increment of alternative current (AC). (c) 2008 Elsevier Ltd. All rights reserved.

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