Elucidating conductivity-permselectivity tradeoffs in electrodialysis and reverse electrodialysis by structure-property analysis of ion-exchange membranes
Graphical abstract
Introduction
Ion-exchange membranes (IEMs) are charged polymeric films that allow the selective transport of oppositely-charged species (counterions), while retaining the like-charged ions (co-ions) and water [1]. IEMs are employed in environmental and energy technologies, such as desalination, fuel cells, and salinity gradient power generation [2], [3], [4], [5], and also chemical production by the chloralkali process [6]. In electrodialysis (ED) desalination, the application of an electric current drives the separation of ions from saline brackish water, across the IEMs, to produce freshwater [2], [7]. Reverse electrodialysis (RED), the power generation analog of ED, converts the chemical potential energy stored in salinity gradients to useful electrical work by the directional permeation of ions across the charge-selective membranes [8], [9]. In both ED and RED, permeability of the IEM to ions and charge selectivity are principal parameters that determine performance.
A tradeoff relationship between permeability and selectivity exists for membrane processes of gas separation, reverse osmosis, and ultrafiltration [10], [11], [12], [13], [14]. Empirical evidence from recent studies indicates IEMs are also bound by a similar constraint — an increase in ionic conductivity (i.e., permeability) is almost inevitably accompanied by a decrease in selectivity for counterions over co-ions, termed permselectivity [5], [15], [16]. Because of this conductivity-permselectivity tradeoff for ion-exchange membranes, any efforts to improve separation will be at the expense of reduced kinetics, thus restricting overall ED and RED performance and energy efficiency [5], [15], [16], [17]. As such, the tradeoff phenomenon has profound impacts on ED, RED, and other IEM-based processes.
Fundamental understanding of the tradeoff and its intrinsic relation to membrane properties is crucial to inform the development of better membranes. However, while theoretical explanations for the tradeoff of other membrane processes are available [10], [11], [12], [13], [14], a complete fundamentals-based framework to describe the IEM conductivity-permselectivity relationship is lacking. Although recent experimental studies demonstrated that membrane water uptake and bulk solution concentrations can induce the tradeoff between IEM conductivity and permselectivity, the qualitative explanations provided do not give a rigorous mechanistic explanation of the phenomenon [15], [18]. Analytical approaches to describe the effects of membrane property on IEM transport are almost always focused on quantifying isolated property-performance relationships [19], [20], [21] (such as, ionic conductivity dependence on bulk concentrations) and oftentimes adopt semi-empirical models, i.e., employ fitting parameters [18], [19], [22], [23]. Hence, such approaches are unable to elucidate the intrinsic relationship between membrane properties and the intertwined performance parameters of permselectivity and conductivity. The Nernst-Planck framework is commonly used to describe IEM transport [21], [24], [25], [26], [27], but requires the activity and diffusion coefficient of ions within the charged IEM matrix, which are anticipated to deviate significantly from bulk solution due to non-idealities and are also not readily accessible by experiments [24], [25]. Recently, studies showed that counterion condensation theory, originally established for aqueous polyelectrolyte solutions, can be applied to IEM to predict ion activity and diffusivity with reasonable accuracy [28], [29], thus highlighting the potential to overcome the present limitations of Nernst-Planck transport models.
This study analyzes ion transport across IEMs to elucidate the dependence of key performance parameters, ionic conductivity and charge selectivity, on intrinsic membrane chemical and structural properties. Firstly, the working principles of ion-exchange membranes, electrodialysis, and reverse electrodialysis are described. The IEM model is presented and principal governing equations are discussed. In the model, ion transport is driven by chemical and electrostatic potential, i.e., the Nernst-Planck equation, and counterion condensation theory is incorporated to account for ion activity and diffusivity within the membrane matrix. Computational codes numerically solve for the system of nonlinear differential equations. After the model is validated with literature data, the effects of operating parameters, electric potential difference and external solution concentrations, on current efficiency and resistance to ion fluxes are examined. The analysis then assessed the dependence of permselectivity and conductivity in ED and RED on the intrinsic membrane properties of ion-exchange capacity, degree of swelling, and membrane thickness. The underpinning phenomena relating operating conditions and membrane properties to IEM performance are highlighted and the principal factors governing the observed conductivity-permselectivity tradeoff are elucidated. Lastly, the implications for ED desalination, RED salinity gradient power generation, and membrane development are discussed.
Section snippets
Working principles of ion-exchange membranes
Ion-exchange membranes are water-swollen polymeric films of typically 50–200 μm thickness, with a high density of charged ionic functional groups fixed to the backbone chains [1], [30], [31]. The selective transport of IEMs is achieved by the charge exclusion principle: the fixed functional groups exclude like-charged co-ions and the membrane preserves electroneutrality by having a high concentration of counterions (opposite charge to fixed moieties). Ion transport is driven by electrochemical
Transport model for ion-exchange membranes
In this section, the transport model for ion permeation in IEMs is presented and key equations are listed. The model considers the solution-membrane interface to be at quasi electrochemical equilibrium and uses the modified Nernst-Planck equation to describe ion fluxes within the membrane matrix under an electrochemical potential gradient. Manning’s counterion condensation model is utilized to account for ion activities and diffusion coefficients within the membrane matrix, which differ
Concentration and electric potential profile
The boundary concentrations of counter- and co-ions are governed by chemical potential equilibrium and electroneutrality at the interface between the membrane and HC and LC solutions, Eqs. (3), (8), respectively. At steady-state, ion fluxes Jct and Jco are constant, and the concentration and electric potential profiles can then be numerically determined using the modified Nernst-Planck equation, Eq. (11), with the boundary condition concentrations. Fig. 2B shows representative cct, cco, and φ
Influence of operating parameters on resistance and current efficiency
Here, the effects of operating parameters, applied voltage and bulk solution concentrations, on membrane performance in ED and RED are examined. Simulated membrane properties of cfix = 1.68 eq/L, fw = 0.30, l = 100 μm, and ξ = 1.08 are held constant throughout this section.
Conductivity-permselectivity relationships as a function of IEM properties
Because ion-exchange capacity, swelling degree, thickness, fixed charge density, and water volume fraction of IEMs are intricately linked [30], [53], experimental approaches to investigate the impact of a single parameter on ED and RED are inevitably confounded by other properties that are simultaneously altered. On the other hand, the analytical framework employed in this study enables the influence of individual intrinsic membrane properties to be isolated for systematic examination. As such,
Implications for ED desalination, RED energy production, and membrane development
This study presents an IEM transport model that employs counterion condensation theory to analytically determine the experimentally inaccessible parameters of ion activity and diffusivity, and overcome a critical limitation hindering the application of the Nernst-Planck framework within the membrane matrix. The approach utilizes only intrinsic membrane properties, i.e., without additional fitting parameters, to determine process performance parameters that are in good agreement with reported
Acknowledgements
We acknowledge financial support from the United States Bureau of Reclamation, Grant R16AC00124. In addition, we thank Dr. Alan C. West and Jonathan D. Vardner for the helpful discussions.
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