Abstract

Ion transport in polyelectrolyte membranes (charged hydrogels) is of significant technological (and biological) importance, but little is known of how micro-structural inhomogeneity affects ionic conductivity. Whereas a uniform electric field drives uni-directional electro-migrative and electro-osmotic ion fluxes in perfectly uniform microstructures, this study considers the influence of spherical inclusions/cavities on the hydrodynamic and ion permeability of charged hydrogels. Such cavities have a high permeability, but they can bear a much lower conductivity due to the partitioning of counter-ions between the cavity and bulk hydrogel phases, also inducing micro-scale electro-osmotic flow. To understand these, perturbations from a nonlinear Poisson–Boltzmann equilibrium state are used to compute the velocity disturbances, and electrostatic and ion-concentration polarization. These furnish three independent Onsager coefficients: one of which is the effective hydrodynamic permeability, and all of which contribute to the two principal electrical conductivities (distinguished by electrode configuration). Cavities with diameters in the range$10$–$1000$ nm are found to be readily polarized, decreasing the effective conductivity of an otherwise uniform polyelectrolyte. In highly permeable hydrogels, however, electro-osmosis may enhance the electrical conductivity when flow is blocked by impenetrable electrodes. Explicit formulas for the hydrodynamic permeability are provided, complementing a simplified (Maxwell–Donnan) analysis of the conductivity, which neglects diffuse double-layer effects and ion-concentration perturbations.

Highlights

  • Hydrogels have traditionally been adopted for biological applications, but are emerging as platforms for a variety of other technologies, including energy storage, 936 A27-1R.J

  • These results are focussed on hydrogels with a low hydrodynamic permeability ( = 1 nm) with negligible added salt, but systematically varying the hydrogel charge density ρf∞ and cavity radius R

  • Having established the principal physical features emerging from the general framework, the sub-sections briefly elaborate by examining responses with higher hydrodynamic permeability (§ 3.3, = 100 nm), and with added salt and intermediate hydrodynamic permeability (§ 3.4, nCl− = 1 mM, = 10 nm)

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Summary

Introduction

Hydrogels have traditionally been adopted for biological applications, but are emerging as platforms for a variety of other technologies, including energy storage,. For relatively weak hydrogels (having low stiffness and high water content), the ‘pores’ are significantly larger than the small ions contained within Such hydrogels readily transport small ions, as evidenced, for example, by the electrical conductivity of polyacrylic acid (anionic) hydrogels (Kuhn mesh sizes ξ ∼ 5–20 nm) being comparable to those of the electrolyte ions within (Adibnia, Afuwape & Hill 2020). This analysis completely neglects ion diffusion and advection, but later serves as a benchmark with which to assess the full electrokinetic model, especially the role of electro-osmosis.

Theory
Electrokinetic model
Averaged current density
Onsager relationships
Numerics
Donnan–Maxwell model
Results
Perturbations from equilibrium in the low-permeability limit
Perturbations from equilibrium in the highly permeable limit
Perturbations from equilibrium at intermediate permeability with added salt
Experimental interpretation
Summary and conclusions
Full Text
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