Introduction

Membrane technology has attracted increasing attention of researchers especially in progressive engineering fields such a solar cells [1], full cells [2], batteries/capacitors [3], and electrodialysis [4]. Polyvinylchloride-based cation-exchange heterogeneous membranes have been widely used in electrodialysis processes on account of obvious advantages such as favorable electrochemical properties, wide availability, low price, and high mechanical, thermal, and chemical stability [46]. Sulfonated polyvinylchloride (SPVC) is SO3-functionalized derivative of polyvinylchloride (PVC) polymer with improved properties such as flexibility, durability, and reactivity when compared with the soft PVC [68]. Sulfonate functionalities not only can elevate the ion-exchange capacity of the PVC but also provide superior conditions for subsequent chemical modifications if necessary [9]. Moreover, more stabile attachment of polymer coatings to the SPVC would be obtained as a result of higher reactivity and increased hydrophilicity of the SO3-functionalized polymer.

Nanoparticles have been extensively utilized to enhance the ion-exchange membrane properties such as chemical reactivity, reusability, mechanical durability, thermal resistance, and chemical stability [5, 1014]. Among popular nanomaterials, nanometal oxides (NMOs) have emerged as highly desirable nanofiller modifiers. NMOs can play important roles in modifying ion-exchange membranes due to their high adsorption capacity, anti-fouling impact, cross-linking mediation, favorable conductivity, biodegradability, and biocompatibility [5, 10, 13]. Titanium dioxide (TiO2), zinc oxide (ZnO), iron oxides (Fe2O3 and Fe3O4), and iron-nickel oxide nanoparticles are examples of NMOs frequently addressed in literature [5, 10, 13, 15].

NMOs can be either incorporated into the polymeric casting solution to obtain mixed-matrix membranes (MMM) or introduced into the coating solution to modify the membrane surface [16, 17]. The latter modification strategy can be carried out through two distinct ways: perfect coating of modifying layer or local patches of coating material [17]. Internal mass transfer resistances may be somewhat increased when perfect dip-coating is of interest. On the other hand, enhancements in separation performance may not be so convincing by using local coating strategy. Electrochemical properties of cation-exchange membranes can be improved by amino-modification of surface [16, 17]. Amino-functionalization can increase the reactivity of the ion-exchange membrane surface. Enhancement of Donnan potential and water affinity are also attainable by amino-functionalization.

Chitosan (CS) is a biopolymer with broad application in affinity-induced separation processes such as adsorption, chromatography, and ion exchange. Popularity of chitosan is mainly for its favorable hydrophilicity, reactivity, mechanical properties, film-forming capacity, and biocompatibility. CS is a multi-functional hydrophilic polymer with abundant reactive –OH and –NH2 functional groups. These functionalities can readily interact with the ions at the membrane surface and enable the polymer to favorably adsorb metal ions from aqueous environment [1720]. Electrical conductivity of chitosan is not relatively high; however, this polymer can favorably chelate the ions from aqueous environment.

To our knowledge, ion-exchange membranes made of sulfonated PVC have not been ever modified with chitosan solution and iron oxide nanoparticles. The aim of the current study is to study the impacts of chitosan coating as well as nano-Fe3O4 incorporation into the casting solutions on the electrodialysis performance of the SPVC membranes. Membranes were characterized by using scanning electron microscopy (SEM) microphotography and Fourier transform infrared spectroscopy (FTIR) spectral analysis. Electrochemical properties of the nanocomposite membranes including ionic permselectivity, permeability, and areal resistance were examined using an electrodialysis setup with NaCl solution as model electrolyte.

Experimental methods and materials

Chemicals

Polyvinylchloride (PVC, S-7054, supplied by BIPC, Iran) and tetrahydrofuran (THF, 72.11 g/mol, 0.89 g/cm3, Merck, Germany) were employed as body polymer and solvent, respectively. Cation-exchange resins (ion exchanger Amberlyst® 15, strongly acidic cation exchanger, H+ form—more than 1.7 mEq/l) and iron oxide nanoparticles (Fe3O4, nanopowder, mean size ∼60 nm, SSA >55 m2/g, 213.53 g/mol) were obtained from Sigma-Aldrich (USA). Chitosan powder (CS, 100,000–300,000 g/mol, 90 % deacetylated) and polyethylene glycol (PEG, 400 g/mol) were purchased from Acros (USA). All other chemicals were of analytical grades and used as received. Distilled water was used throughout the experiments.

Membrane preparation

Sulfonated polyvinylchloride was prepared by oxidation of soft polyvinylchloride through batch recirculation with concentrated sulfuric acid. Sulfonation process was carried out according to the procedure proposed by Xu and Kee Lee [7]. Afterwards, SPVC was utilized as the main polymer for the preparation of cation-exchange membranes.

Support preparation

At first, pristine SPVC membranes were fabricated on the basis of the phase inversion technique. The pristine SPVC membranes were then used as support for the preparation of nanocomposite membranes. Distinct amount of SPVC polymer was dissolved in THF solvent under rigorous stirring (stirrer model: Velp Sientifica Multi 6, USA) for around 7 h. Afterwards, resin particles (−300 + 400 meshed) were introduced into the polymeric casting solution and sonicated for 1 h using ultrasound bath (SONREX Digit DT52 H, BANDELIN, 240 W, 35 kHz, Germany). After a short period of magnetic restirring, the polymeric solution was casted on clean glass plates using an appropriate applicator. Afterwards, the membranes were dried at room temperature followed by immersing in distilled water as non-solvent agent. Finally, the membranes were soaked in 0.5 M NaCl solution for 48 h to be fully saturated before application in electrodialysis experiments. Membrane thickness was measured using a digital micrometer device (electronic outside micrometer, IP54 model OLR, Lianyungang Linuo Co., China).

Surface modification

Nanofiller-free casting solution was prepared by dissolving 2 wt% chitosan, 1 wt% polyethylene glycol (as porogen), and 1 wt% acetic acid in DI water under vigorous stirring. Nano-Fe3O4-added casting solutions were prepared by introducing different amounts of Fe3O4 nanoparticles into the soft CS casting solutions. Nanofiller-added casting solutions were ultrasonicated for around 0.5 h for the desired dispersion of the nanoparticles just before surface modification. Precise slices of SPVC membranes were moisturized and then pasted on clean glass plates for coating. Casting solution was poured onto the surface of the membrane samples and then exactly casted using an applicator with pre-determined gap size of 450 μm. Afterwards, the modified membranes were air-dried for 24 h at room temperature and then soaked in 0.5 M NaOH for 1 h to neutralize the excess acid and crosslink. Finally, the resultant membranes were rinsed with abundant distilled water and saved in 0.5 M NaCl solution for subsequent electrodialysis experiments. Briefly, composition of the resultant membranes is addressed in Table 1.

Table 1 Composition of coated SPVC cation-exchange membranes

Electrodialysis setup

Electrochemical transport properties of the prepared membranes were examined using a typical two-compartment electrodialysis test cell. The setup has been explained in details elsewhere [46]. The membrane sample was sandwiched between the two half-cells and exactly sealed. The half-cells were equipped with platinum electrode supported with a Teflon cover sheet on one side and a porous support for the membrane on the other side. Solutions in both sections were vigorously stirred by magnetic stirrers (in the vicinity of the membrane) to minimize the external mass transfer resistances. The setup was also equipped with electrical power supplier and online data acquisition system.

Membrane characterization

Scanning electron microscopy

Cross section morphology of the membranes was investigated by using Philips-X130 and Cambridge scanning electron microscopes. In brief, membrane specimens were frozen in liquid nitrogen. Afterwards, the samples were broken and air-dried. The prepared samples were gold sputtered for taking the micrographs in vacuum conditions.

Fourier transform infrared spectroscopy

Fourier transform infrared spectroscopy (FTIR) spectral analysis was carried out to specify the functional groups of the polymers and membranes. An ABB Bomem FTIR spectrometer (MB-104) was applied for this purpose.

Permselectivity

Membrane potential includes Donnan and diffusion potentials [7, 8]. Ionic permselectivity was computed for the equilibrated membranes by using unbalanced concentrations of NaCl electrolyte solution (C 1 = 0.1 M, C 2 = 0.01 M) on different sides of the membrane in electrodialysis cell. Electrical potential developed across the membrane was monitored by connection of either half-cells to a digital auto multi-meter (DEC, model: DEC 330FC, Digital Multimeter, China) and using saturated calomel electrode through KCl bridges. The membrane potential (E M) is represented by the well-known Nernst equation [21, 22] as

$$ {E}_{\mathrm{M}}=\left(2{t}_{\mathrm{i}}^{\mathrm{m}}-1\right)\left(\frac{RT}{n\ F}\right)\ \ln \left(\frac{a_1}{a_2}\right) $$
(1)

where t i m is the transport number of counterions in the membrane phase, R is the universal gas constant, T is the absolute temperature, n is the electrovalence of counterions, a 1 and a 2 are the activities of electrolyte solutions in contact with the membrane surfaces, and F is the faraday constant. The ion permselectivity of the membranes is represented for the electromigration of counterions through the ion-exchange membrane and given by the following equation [23]:

$$ {P}_{\mathrm{s}}=\frac{t_{\mathrm{i}}^{\mathrm{m}}-{t}_0}{1-{t}_0} $$
(2)

where, t 0 is the transport number of counterions in the receiver solution, i.e., solution to that the ions migrate from the feed [2123].

Ionic permeability

Of the setup, 0.1 M NaCl solution was poured in one half-cell and 0.01 M NaCl solution on its other half-cell to measure the ionic permeability of the membranes. DC electrical potential source (Dazheng, DC power supply, Model: PS-302D) with a constant voltage was used across the cell with stable platinum electrodes. Cations can pass through the membrane to appear in cathodic section. Based on the Fick’s first law, flux of the ions can be expressed by [47, 23]

$$ N=-\frac{V}{A}\times \frac{d{C}_1}{dt}=P\frac{C_1-{C}_2}{d} $$
(3)

where P is the diffusivity of ions, d is the membrane thickness, A is the membrane effective area, V is the volume of the solution, C i is the cation concentration in the half-cells, and N is the ionic flux. Eq. (4) is obtained by integration of Eq. (3) as follows:

$$ \ln \frac{\left({C_1}^0+{C_2}^0-2{C}_2\right)}{\left({C_1}^0-{C_2}^0\right)}=-\frac{2 PAt}{Vd} $$
(4)

where

$$ {C_1}^0=0.1\kern0.5em \mathrm{M},{C_2}^0=0.01\kern0.5em \mathrm{M},{C}_1+{C}_2={C_1}^0+{C_2}^0=0.11\kern0.5em \mathrm{M} $$
(5)

Diffusion coefficient (P) can be calculated by using Eq. (4), where pH variation in cathodic section is being monitored using a digital pH meter (Jenway, model: 3510). Accordingly, flux of the cations can be calculated using Eq. (3).

Areal resistance

Electrical resistance of the equilibrated ion-exchange membranes was measured in 0.5 M NaCl solution at ambient temperature. The current bridge was being altered with 1500 Hz frequency (audio signal generator, Electronic Afzar Azma Co. P.J.S) to measure the resistance. The areal resistance was represented by [22]

$$ r={R}_{\mathrm{m}}\times A $$
(6)

where r is the areal resistance, R m is the different between the cell resistance and the electrolyte solution resistance, and A is the membrane surface area.

Results and discussion

Morphology and chemistry

SEM image from the cross section of the plain SPVC membrane is depicted in Fig. 1a. Figure 1b presents the cross section of the CS-coated membranes. The chitosan coating layer with the thickness around 5 μm is obvious in Fig. 1b. Cross section of the CS-coated membranes with 2 wt% Fe3O4 nanoparticles in the coating layer is shown in Fig. 1c. As it is clear in Fig. 1c, CS layer not only covers the membrane surface homogeneously but also scaffolds the resin agglomerates inside the SPVC membrane matrix. In addition, the coating layer becomes relatively porous as a result of the nanofiller insertion. Microvoids are obvious in chitosan layer in Fig. 1c. It is confirmed by other researchers that morphology plays a pivotal role in electrotransport properties of conductive membranes [24].

Fig. 1
figure 1

Cross section SEM images of a pristine SPVC membrane, M (×1000 and scale bar 30 μm), b CS-coated SPVC membrane, M0 (×500 and scale bar 30 μm), and c CS/Fe3O4-coated membrane, M2 (×500 andscale bar 30 μm)

Figure 2 shows infrared spectra of PVC and SPVC, respectively. In the measurement results of the soft PVC, the peaks in the vicinities of 1,425, 959 and 610 cm−1 are peaks originating from the PVC. In many infrared spectra of soft PVC, verification of PVC is accomplished using the C–Cl stretching vibration near the wavelength of 610 cm−1. In SPVC spectra, the peaks which appeared around 1030 and 1100 cm−1 are ascribed to the symmetric and asymmetric stretching vibration of the sulfonic acid groups [7].

Fig. 2
figure 2

Infrared spectra of polyvinyl chloride and sulfonated polyvinyl chloride polymers

Figure 3 exhibits infrared spectra of pure CS-coated membrane (M0) and CS-coated membrane containing 2 wt% Fe3O4 nanoparticles (M2). The peak around 3440 cm−1 observed in both curves was ascribed to the vibration of the hydroxyl groups. In the spectrum of CS (Fig. 3 (a)), the absorption bands which appeared at 1589 and 1399 cm−1 can be assigned to the N–H bending vibration and C–O stretching bonds of the primary alcohol groups in chitosan polymer. By comparing the infrared spectra of Fe3O4–chitosan-coated membranes (Fig. 3 (b)) with that of the pure CS-coated membrane, one can obtain that the 1589 cm−1 peak of the N–H bending vibration shifts to 1562 cm−1. Moreover, a new peak which appeared at 560 cm−1 connects to the Fe–O group stretching vibrations [25].

Fig. 3
figure 3

Infrared spectra of (a) CS-coated SPVC membrane (M0) and (b) CS/Fe3O4-coated SPVC membrane (M2)

Permselectivity

Selectivity of the cation-exchange membranes originates from the charge that the membrane matrix carries [26]. Result of the NaCl permselectivity through the membranes is depicted in Fig. 4. Results indicate that membrane selectivity is enhanced by coating CS layer. As it is clear in the SEM images, the CS layer covers the membrane surface as well as the resin agglomerates inside the membrane structure for M0 and M2. Chitosan layer can reduce external mass transfer resistances in the vicinity of the membrane surface. Therefore, the ion uptake rate to the membrane surface increases. This may be attributed to the function of the amino and hydroxyl groups of chitosan polymer. Moreover, the membrane surface is provided with more negative charge by hydrolysis of these functional groups. This causes better exclusion of the co-ions (ions of the same charge as the membrane charge) from the membrane surface. Intensification of Donnan potential near the membrane surface resulted from the enhanced exclusion of the co-ions. This fact is the main reason for the improvement of the membrane selectivity. In addition, CS-coated resins can facilitate the transport of the counterions through the membrane matrix [27]. Membrane hydrophilicity is also enhanced as a result of chitosan coating. Thus, the accessibility of the counterions to the fixed sites is facilitated. This also positively affects the transport of the counterions through the membrane [28].

Fig. 4
figure 4

Permselectivity of the SPVC cation-exchange membranes with CS coating layer comprising different values of Fe3O4 nanoparticles

Permselectivity of sodium chloride was further enhanced by introduction of iron oxide nanoparticles in the CS coating layer up to 2 wt%. Membrane selectivity was decreased with further nanoparticle incorporation (from 2 to 4 wt%). Selectivity enhancement may result from the magnetic and adsorptive characteristics of Fe3O4 nanoparticle toward counterions. Moreover, insertion of Fe3O4 into the CS layer can also reduce resistances against transfer of counterions. The observed reduction in the permselectivity at 4 wt%, however, may be attributed to the clogging of the ionic transport pathways. Clogging may be caused by agglomeration of the nanoparticles at high loading contents, as addressed by other researchers [5, 10, 11, 14]. Agglomeration limits the accessibility of the counterions to the reactive sites and thus facilitates the permeation of the co-ions through the membrane. Moreover, increased affinity of Fe3O4 nanoparticles at high additive loading provides the conditions for superior interaction of the ions with the membrane surface. This improves the percolation of the co-ions through the membrane as a result of the concentration gradient development across the membrane.

Ionic permeability

Permeability of the membranes was improved as a result of the surface modifications (Fig. 5). CS coating layer resulted in ionic flux increase on account of Donnan potential enhancement. Moreover, abundant hydroxyl and amine groups of chitosan are responsible for this behavior [17, 2931]. Superior monovalent permeability was also obtained by Wang et al. [32], after immobilization of chitosan layer to the bare cation-exchange membrane. Membrane with more negative surface charge can superiorly repel back the co-ions from the membrane surface. Flux of Na+ ions is also enhanced by the increase of Fe3O4 nanoparticles content in the CS layer. This may be attributed to the adsorptivity of Fe3O4 nanoparticles which strengthens the interactions of the functional sites with the cations [27, 30]. So, the transport of the ions is facilitated in presence of the nanometal oxide. Moreover, the electromagnetic impact of Fe3O4 is also another reason for the permeability improvement. This property causes electrical potential field enhancement across the membrane.

Fig. 5
figure 5

Ionic permeability of the CS/Fe3O4 modified SPVC cation-exchange membranes

Areal resistance

The areal resistance experiment is a performance test accompanied with high experimental fluctuations even after many replications. To report meaningful data, only plain SPVC membrane has been compared with the optimal membrane (M2), in this regard. The areal electrical resistance of the optimal and pristine membranes is compared in Fig. 6. It is obvious that the areal resistance is reduced from 9.4 (ohm) in plain membrane to 2.9 (ohm) in CS/Fe3O4-coated membrane. The electrical resistance is obviously reduced with the help of the CS coating layer and Fe3O4 nanoparticles. This is ascribed to the enhancement of the membrane properties as a result of the CS/nanofiller synergy.

Fig. 6
figure 6

Areal resistance of the M (pristine SPVC) and M2 (CS/Fe3O4) modified SPVC cation-exchange membrane

Electromagnetic and adsorptive properties of Fe3O4 nanoparticles can also strengthen the interactions of the ions with the membrane surface. Additionally, Fe3O4 as an efficient mediator for electron transfer can increase the conductivity of the membranes [3133]. Synergetic effects of CS and the nanofillers would result in enhancement of the electrical potential field across the membrane.

Conclusions

SPVC heterogeneous cation-exchange membranes were synthesized and then modified with chitosan layer comprising various amounts of Fe3O4 nanofillers. CS layer could enhance electrochemical properties of the membranes by the introduction of plentiful reactive sites on the surface. The ionic flux and permselectivity of the membrane was enhanced by increasing the nanoparticles from nil to 2 wt%. The electrochemical properties were not improved by further additive insertion due to disadvantages of the nanofiller agglomeration. Thus, the optimum nanoparticle content in the CS layer was obtained as 2 wt%. Areal resistance of the membranes was also reduced by CS/Fe3O4 surface modification. Generally, the results indicated that the SPVC membranes modified by CS/Fe3O4 coating are potential candidates for electrodialysis processes.