Home Preparation of a poly(DMAEMA-co-HEMA) self-supporting microfiltration membrane with high anionic permselectivity by electrospinning
Article Open Access

Preparation of a poly(DMAEMA-co-HEMA) self-supporting microfiltration membrane with high anionic permselectivity by electrospinning

  • Henmei Ni EMAIL logo , Yadong Yang , Yixuan Chen , Junxiu Liu , Lijuan Zhang and Min Wu
Published/Copyright: October 18, 2016
Become an author with De Gruyter Brill

Abstract

A cross-linked microfibrous anion exchange membrane with high ion permselectivity and robust mechanical properties was fabricated by electrospinning. Copolymer, poly N,N-dimethylaminoethyl methacrylate (DMAEMA)-co-2-hydroxyethyl methacrylate (HEMA), was selected as the electrospun material. Fourier transform infrared (FTIR) spectroscopy, 1HNMR and scanning electron microscopy (SEM) were employed to characterize the copolymer and microfibrous mat. The electrospinning optimal parameters were determined by orthogonal experiments. Formaldehyde vapor was applied to crosslink the mat. It was observed that the water sorption decreased from 75.7% to 30.4% as the crosslinking time increased from 20 h to 32 h. The robust mat with the high tensile strength of 4.62 MPa and 50% elongation at break was obtained at 24 h. The ion permeability of NO3, Cl, SO42− were 94, 91 and 87%.

1 Introduction

The treatment of brackish water, waste water and seawater into clean water is an effective approach to tackle the scarcity of fresh water and relieve the environmental stress. Various technologies such as membrane distillation, electrodialysis, freeze desalination and nanofiltration, etc., have been developed. Among them, nanofiltration is now emerging as a viable alternative to conventional water treatment because it can operate at the lower pressure, provide high flux and is more energy efficient (1). The nanofiltration membrane usually comprises three fundamental layers: 1) top ultra-thin selective barrier layer, 2) middle porous support and 3) bottom non-woven fabric. The top ultra-thin layer plays the main role in the separation. Conventionally, amide or imidazolium functional groups are usually selected as the active groups providing the ion selectivity to membrane due to their positive charges. In order to ensure the water flux, the layer must be porous and high crosslinked to resist the solution of materials. Hence, a electrospinning fibrous mat is viable to be the support membrane for the active materials due to its high ratio of surface area to volume, tailorable pore sizes and flexibility in surface chemistry (2), (3), (4). For example, Wang et al. successfully introduced the crosslinked polyvinyl alcohol (PVA) microfibrous mat into the structure of nanofiltration membranes (5), (6). Yoon et al. used a poly(acryl nitrile) (PAN) microfibrous mat to enhance the mechanical strength of the top thin layer (7). However, a disadvantage is obvious, namely loading the active materials on the microfibrous mat. Interfacial polymerization is commonly employed to combine the active materials into nanofribrous mat. It is complicated and hard to control the layer thickness and uniformity of the surface reaction. For example, the permselectivity of specific anion is regulated mainly by the balance of hydration energy of anions and the hydrophilicity of membranes (8). It is revealed that the permselectivity between two anions is strongly dependent on the hydrophilicity, namely that with the decrease of hydrophilicity, the permeation of less hydrated anions increases. Moreover, the pseudo-grafted active materials may come off in the application in turn to shorten the life-span of membrane. Hence, it is necessary to fabricate a membrane with uniform surface chemistry.

In addition, the weak mechanical strength of the microfibrous mat needs a supporting material. Porous polysulfone membrane is commonly applied. However, the thickness and pore size of polysulfone membrane greatly affect the water flux. In order to solve the problem, Satinderpal et al. explored a concept called a self-supporting barrier layer by using the strong poly(vinylidene fluoride) (PVDF) microfibrous mat (9), (10). This concept recently has attracted increasing interest from researchers. For example, Prince et al. added the nano clay particles (11) and SiO2 nanoparticles (12) into PVDF to improve both the mechanical strength and hydrophilicity of PVDF microfibrous mats. Wang et al. promoted the strength of the membrane by transforming PAN nanofibers into carbon nanofibers (13). Recently, Jiang et al. further enhance the strength by using polyimide as the nanofiber material (14). However, improved water flux and solute rejection were achieved by a nanofiltration membrane, it is prone to fouling, non-selective and energy consuming. Hence, it is necessary to develop a new approach for the fabrication of nanofiltration membranes.

In this paper, a new approach was developed to fabricate the self-supporting barrier layer of a nanofiltration membrane. As shown in Scheme 1, the water soluble copolymer of poly N,N-dimethyl amino ethylene methacrylate (DMAEMA) and co-2-hydroxyethylene methacrylate (HEMA) were selected as the materials of both the barrier layer and the mechanical supporting membrane. These were electrospun into nanofibers and then crosslinked with formaldehyde vapor. Finally, the tertiary amino groups were transformed into a quaternary amine salt by CH3I. Both the DMAEMA and HEMA are hydrophilic, thus the membrane is hydrophilic. Moreover, the active material is uniformly and chemically bonded on the supporting matrix. Furthermore, the quaternary amine salt is a well-known anti-microbial agent (15), (16), thus it can protect the membrane from biofouling.

Scheme 1: Process of fabricating the self-supporting microfiltration membrane by electrospinning.
Scheme 1:

Process of fabricating the self-supporting microfiltration membrane by electrospinning.

2 Experimental

2.1 Materials

The monomers, HEMA (analytic grade), DMAEMA (analytic grade), were obtained from Aldrich. The monomers were purified by distillation under the reduced pressure. Other reagents, such as 2, 2′-azobis (isobutyronitrile) (AIBN, chemical grade), N, N′-dimethylformamide (DMF, analytic grade), methanol and diethyl ether, were purchased from Guoyao Chemicals Co. Ltd. (Beijing, China) and used as received. Distilled water (DI) was used throughout the experiment.

2.2 Synthesis of poly(DMAEMA-co-HEMA)

The ratios of HEMA/DMAEMA (w/w) were 2/1, 4/1, 5/1 and 6/1. As an example, the process of copolymerization with HEMA/DMAEMA=4/1 was described as follows: HEMA (8.0 g), DMAEMA (2.0 g) and methanol (85 ml) were added into a 150 ml three-necked flask equipped with an inlet for a condenser, an inlet for a thermometer and an inlet for the charging reagents. The mixture of reagents was purged with N2 to deoxygenate for 30 min at room temperature. Afterwards it was heated to 60°C, AIBN (0.1 g) dissolved in 5 ml methanol was added. The polymerization was carried out at 60°C with a magnetic stirrer for 10 h, wherein positive N2 pressure was maintained throughout. The resulting solution was then precipitated by adding diethyl ether, and the copolymer was dried in a vacuum oven at 60°C for 24 h.

The copolymer was characterized by 1H NMR spectroscopy (AVANCE AV-500, Bruker Ltd. Co., Britain) with CDCl3 as a solvent and Fourier transform infrared (FTIR) spectroscopy (NICOLETAVATAR 370, Nicolet Ltd. Co., Tokyo, Japan) by using a KBr tablet as a sample loader. The thermal property of copolymer was investigated with a differential scanning calorimeter (DSC8523, Rigaku Co. Ltd., Tokyo, Japan) in N2 atmosphere. The scanning rate was 20°C/min.

2.3 Preparation of an anion exchange membrane by electrospinning

Poly (DMAEMA-co-HEMA) was dissolved in DMF to produce various spinning solutions. The equipment and operation are described elsewhere (17).

The as-prepared nanofiber was evaluated by scanning electron microscopy (SEM) (JSM-5310, JEOL, Tokyo, Japan). The diameter of nanofiber was calculated from the SEM photos (17), (18). The photos were magnified 10 fold at first and then printed. The diameters of about 100 microfibers were selected and measured with an ordinary ruler. The error was about 0.5%.

2.4 Crosslinking the membrane and quaternization of the amines

Quaternization of amine groups was performed analogous to staining the sample of the amino substance with iodomethane vapor for transmission electron microscopy (TEM) (17), (18). The membrane (40×40 mm) was placed on a scaffold settled in a 100 ml beaker. Three milliliters of CH3I was poured into the beaker without flooding the membrane, and then the beaker was sealed with plastic film. The quaternization of amine was conducted in the dark at room temperature for a week. As for the crosslinking reaction, the apparatus and device were the same as described above, except that a 500 ml beaker was used. A hundred milliliters of formaldehyde aqueous solution (30%) was charged into the beaker without flooding the membrane, and then the beaker was sealed with a plastic film (19). The beaker was placed in a water bath and the crosslinking reaction was carried out at 60°C.

2.5 Water sorption of the anion exchange membrane

The water sorption was equilibrated in deionized water for 12 h. After the excess water on the sample surface was wiped off, the sample was weighed (mwet). The dry weight (mdry) of the sample was determined after drying to a constant weight under a vacuum at 60°C. The water sorption, φw, was calculated as following.

φω=mwetmdrymdry×100%

2.6 Determination of permselectivity

The transport number of gegenions and the value of permselectivity were determined by measuring the membrane potential. We made the equipment used ourselves. Its structure is shown in Figure 1. The size of the plastic cell was φ 30 mm×100 mm. The diameter of the connector was φ 5 mm.

Figure 1: Schematic diagram of equipment for the determination of permselectivity.
Figure 1:

Schematic diagram of equipment for the determination of permselectivity.

Different concentrations of salt, for instance, 0.1 mol/l KCl and 0.2 mol/l KCl, were injected into two cells at 25°C, respectively, and we then measured the potential using a digital potentiometer (SDC-II, Sangli Electronics Co., Nanjing, China). The relation between the membrane potential (Em) and the transport number of gegenion (t¯g) through the membrane are as follows:

t¯g=Em+Em02Em0

where t¯g is the transport number of the gegenion through the membrane, Em0, is the ideal potential (16.1 mV) and Em, is the membrane potential measured. The permselectivity of the membrane was calculated as:

P=t¯gtgtg0¯tg=t¯gtg1tg

where P is the permselectivity, t¯g, is the transport number of gegenion through the membrane and tg, is the transport number of gegenions in the solution found in the relevant manual.

2.7 Mechanical property

The mechanical properties of membranes were tested with a gage length of 50 mm and crosshead speed of 10 mm/min by electronic fiber strength tester (Series IX Automated Materials Testing System, Instron Corporation). Ten samples were tested and the mean values are used in the article. All samples were conditioned in a laboratory environment for 24 h before testing.

3 Results and discussion

3.1 Characterization of the copolymer

Both the DMAEMA and HEMA are the methacrylate ester. Although the copolymerization reactivity ratios of the two monomers were not found, theoretically it is rational that their copolymerization reactivity ratios are similar. Teoh et al. reported that, in the ATRP copolymerization, the copolymerization reactivity ratios of (1) HEMA and (2) DMAEMA were near unity (r1=1.08, r2=1.12) in the polar solvents (20). Therefore, the composition of copolymer was close to the feed ratio of monomers. The random copolymer of P(DMAEMA-co-HEMA) was characterized by FTIR and 1HNMR as shown in Figure 2. The broad peak at 3450 cm−1 was attributed to the vibrations of the hydroxyl groups. A peak at 2932 was assigned to the asymmetric vibration of CH3. A peak at 1650 cm−1 was the typical stretch vibration of the ester carbonyl group. The absorption band at 1190 cm−1 corresponded to the symmetric stretching vibration of C-N band associated with the DMAEMA unit.

Figure 2: FTIR spectra of poly(DMAEMA-co-HEMA).
Figure 2:

FTIR spectra of poly(DMAEMA-co-HEMA).

A representative 1H NMR spectrum of poly (DMAEMA-co-HEMA) in d-CHCl3 is shown in Figure 3. The peak, e.g. (δ=4.1 ppm) belongs to the α-protons of the ester groups in both DMAEMA and HEMA; peak f (δ=3.7 ppm), protons of ethyl groups in HEMA; peak d (δ=2.6 ppm), protons of ethyl groups in DMAEMA; peak c (δ=2.3 ppm) and protons of methyl groups in the tertiary amine of DMAEMA.

Figure 3: 1H NMR spectra of poly(DMAEMA-co-HEMA) in d-CHCl3 with peaks assigned.
Figure 3:

1H NMR spectra of poly(DMAEMA-co-HEMA) in d-CHCl3 with peaks assigned.

A representative DSC diagram of copolymer (HEMA/DMAEMA=4/1) is shown in Figure 4. It is clear that there is only one Tg existing in the figure. The single peak of Tg usually reflects the homogeneous distribution of components in a polymer blend, namely that no domain or phase formed solely by one kind of polymer blocks exists in the blend. In the case that two polymeric units are immiscible, it can be a criterion to prove the formation of copolymer. Therefore, this result indicated that the random copolymer of poly(HEMA-co-DMAEMA) was successfully prepared. Moreover, as shown in Figure 4, Tg was about 320 K. However, Martin-Gomis et al. investigated the bulk copolymerization of HEMA and DMAEMA, and the thermal properties of copolymer with various compositions (21). They reported that Tg of poly(HEMA-co-DMAEMA) with 20% DMAEMA was about 330 K. The difference was likely the result of an experimental error, i.e. the determination of baseline (Figure 4). Anyway, it was not the main intention of this paper to accurately determine the Tg of the copolymer. Therefore, to some extent, Tg of ca 320 K supported the formation of a copolymer with the same composition as the feed ratios.

Figure 4: DSC diagram of copolymer (HEMA/DMAEMA=4/1).
Figure 4:

DSC diagram of copolymer (HEMA/DMAEMA=4/1).

3.2 Determination of the optimal electrospinning parameters

As we know, electrospinning of poly (DMAEMA-co-HEMA) was carried out for the first time in this paper. Therefore, first of all, the electrospinning parameters should be obtained. In the preliminary experiments, it was observed that the microfibers were prepared without beads only when the total concentration of the copolymer was higher than 40 wt%. However, when the concentration was higher than 50 wt%, the distribution of the microfiber diameters became significantly more broad. Moreover, the averaged diameter of nanofibers was overwhelmingly dependent to the concentration, with less regard to the composition of the copolymer. These were the features of electrospinning systems applied in this paper, and also, the reasons that the following parameters were selected for the optimization of conditions to prepare the uniform microfibers.

The quantitative evaluation and statistic analysis of the effects of solution properties and processing parameters were investigated with the orthogonal experiment design. Four relevant factors were investigated: (A) solution concentration, (B) voltage, (C) flow rate and (D) tip to collector distance. Three levels were set for each factor, and the boundary values for the levels were determined in pilot experiments to ensure microfiber formation without droplets. Solution concentrations of 42 wt%, 44 wt% and 46 wt% were used. The feed rates of 0.7, 1.0 and 1.3 ml/h with a syringe pump were employed. The applied voltage ranged from 10 to 14 kV, and the distance from the collector to the needle tip ranged from 12 to 16 cm. All electrospinning experiments were carried out at 25°C and relative humidity of 40%. The surface morphologies of microfibers were examined by SEM. The fiber diameter averaged over at least 100 microfibers was determined by SEM micrographs. The aim of orthogonal experiments was to analyze the major factors affecting the diameter of microfibers by L9 (34) orthogonal table arrangements. The electrospinning parameters of the orthogonal experiment, fiber diameters and its standard deviation are listed in Table 1. As shown in Table 1, K value represented the average of three values at each level for each factor. Rd, Rs2 represents the difference of maximal and minimal microfiber diameters and its standard deviation, respectively.

Table 1:

Orthogonal experimental design and the experimental results.

Exp. no.FactorsAverage diameter (µm)Standard deviation
Concentration A (wt%)Voltage B (KV)Flow rate C (ml/h)Distance D (cm)
142 (1)10 (1)0.7 (1)12 (1)1.7480.050
242 (1)12 (2)1.0 (2)14 (2)2.0840.048
342 (1)14 (3)1.3 (3)16 (3)2.3940.130
444 (2)10 (1)1.0 (2)16 (3)2.3520.048
544 (2)12 (2)1.3 (3)12 (1)2.7520.072
644 (2)14 (3)0.7 (1)14 (2)2.2230.095
746 (3)10 (1)1.3 (3)14 (2)2.4370.077
846 (3)12 (2)0.7 (1)16 (3)2.9290.077
946 (3)14 (3)1.0 (2)12 (1)2.9620.076
K16.2266.5376.9007.462
K27.3277.7657.3986.744
K38.3287.5797.5837.675
k12.0752.1792.3002.487
k22.4422.5882.4662.248
k32.7762.5262.5282.558
Rd0.7010.4090.2270.310
Rs20.0050.0420.0350.019

As shown in Table 1, it was obvious that, for the microfiber diameter, the significance levels are listed in the order: solution concentration >voltage >collector distance >flow rate. According to the results of the range analysis, the solution concentration played the most important role on the fiber diameter. Hence, in order to reduce the average diameter of microfibers, the best combination of the level of each factor was A1B1C1D2 according to the relationship between factors and fiber diameters. However, the standard deviation of microfibers must be taken into account as it represents the uniformity of microfibers. Therefore, overall the best combination was A1B1C2D1. Namely, the proper conditions for electrospinning were: solution concentration, 42 wt%; voltage, 10 kV; flow rate, 1.0 ml/h; tip-collector distance, 12 cm. Under these conditions, the averaged diameter of microfibers was about 1200 nm and deviation was 0.05.

3.3 Membrane characterization

The final experimental microfibrous membrane was obtained with the optimal electrospinning parameters when the electrospinning time was 30 min. As shown in Figure 5A, the as-prepared microfibrous membrane was not directly applied for the separation process because of its loose structure. Accordingly, the microfibrous membrane was fumed in formaldehyde atmosphere at 60°C, so that the microfiber copolymer was crosslinked due to the reaction of hydroxyl groups in HEMA and formaldehyde. Obviously, after being crosslinked, the membrane became denser (Figure 5B). To further elucidate the microscopic structure of the membrane, the typical surface morphologies at pre- and post-treatment were observed by SEM and are shown in Figure 5C and D, respectively. It is clear that the crosslinked microfibers became flat and curved (Figure 5D). Such a structure implies that the crosslinking reaction may occur in both intra-microfiber copolymers and inter-microfiber copolymers.

Figure 5: Optical and SEM photographs before and after crosslinking (A: optical photograph before crosslinking, B: optical photograph after crosslinking, C: SEM photograph before crosslinking, D: SEM photograph before crosslinking).
Figure 5:

Optical and SEM photographs before and after crosslinking (A: optical photograph before crosslinking, B: optical photograph after crosslinking, C: SEM photograph before crosslinking, D: SEM photograph before crosslinking).

3.4 Water sorption

Amino groups of DMAEMA are the active groups in the membrane. Hence, theoretically the more DMAEMA the better performance can be anticipated. In this paper, four molar ratios of monomers were employed to carry out the copolymerization, i.e. HEMA/DMAEMA=2/1, 4/1, 5/1 and 6/1. The difference in diameters of microfibers with these ratios was insignificant because, as discussed above, the diameter was dominantly determined by the concentration. However, the difference in water sorption was very big. As shown in Figure 6, the content of absorbed water decreased as the composition of HEMA increased. Meanwhile, the water sorption decreased with the increase of crosslinking time, regardless of the ratio of the monomers. This result was normal because HEMA mainly provided the hydroxyl groups for the crosslinking. The water sorption of a membrane electrospun with HEMA/DMAEMA=2/1 was not measurable because it almost dissolved in water, even though it was crosslinked for 32 h. These results indicated that the crosslinking reaction occurred in microfibrous membranes because the hydrophilicity decreased with the increase of crosslinking time. It was coincident to the results reported on PVA, although the water sorption in this paper was much higher (8). As we know, the hydrophilicity of anion exchange membranes strongly impacts to the perselectivity of anions, namely that decreasing hydrophilicity of membranes favors the permeation of less hydrated anions. Hence, for the application, the HEMA/DMAEMA ratio of 4/1 was the best and the crosslinking time should be shorter than 28 h.

Figure 6: Water sorption of the cross-linked membranes vs. the crosslinking time.
Figure 6:

Water sorption of the cross-linked membranes vs. the crosslinking time.

3.5 Mechanical properties

The mechanical properties of microfibrous membranes with HEMA/DMAEMA=4/1 were measured and summarized in Table 2. It is clear that the tensile strength and modulus increased with the increase of crosslinking time. The elongation at the break at first increased as the crosslinking time increased from 20 to 24 h, and then decreased with the increase of crosslinking time. These results indicated that the density of crosslinking points in the membrane increased with the increase of crosslinking time. At 24 h, the membrane was the strongest. When the crosslinking time exceeded 24 h, the membrane became more and more brittle. Therefore, it was determined that 24 h was the proper time of crosslinking.

Table 2:

The mechanical properties of membranes with different crosslinking time.

Crosslinking time (h)Tensile strength (MPa)Tensile modulus (MPa)Elongation at break (%)
202.806.8341
244.629.2450
284.8812.8438
325.3022.0824

The mechanical properties of various microfibrous mats (22), (23) or single microfibers (24) have been investigated by many researchers. For example, Wang et al. (5) reported that the tensile strength of PVA microfibrous mat crosslinked with glutaraldehyde in acetone for 24 h was close to 8 MPa, whilst the uncrosslinked one was about 6 MPa. In contrast, the tensile strength of PAN and PVDF microfibrous mats were about 4 and 2 MPa at the break, respectively. The tensile strength of crosslinked PVA was much higher than that of the crosslinked poly (DMAEMA-co-HEMA) microfibrous mat shown in Table 1. However, we must point out, it is not rational to compare the data of tensile strength given in different papers as the mechanical test of the microfibrous mat is dependent on the precise measurement of the section area of the mat. The microfibrous mat is soft and sponge-like. A screw micrometer is usually applied to measure the thickness. However, the contact pressure of the micrometer on the surface of the mat is determined artificially. The difference in pressure gives a different number of thickness. Therefore, in reality the data of tensile strength given by different measurements is not comparable, even though, we think that the different crosslinking methods might result in different strengths. For example, in the reference, the glutaraldehyde could directly contact with the hydroxyl groups in acetone (5). However, in the present paper, the above method was not applicable because the copolymer was soluble in both water and acetone. Hence, the formaldehyde vapor was applied. By this means, the crosslinking reaction was dependent on the condensation and adsorption of formaldehyde in the mat. Reminiscent of the water sorption and big diameter of microfiber, it was possible that the crosslinking reaction mainly occurred on the surface of the fiber. And also, the bigger diameter of nanofiber decreased the density of inter-fiber contact points, in turn decreases the tensile strength. Accordingly, the crosslinking method an be improved in the future in order to further increase the tensile strength.

In the references, microfibrous mat was only applied as the supporting materials (2), (3), (4), (5), (6), (7). The active material was needed to be grafted on the microfibrous mat by interface polymerization. Therefore, comparatively, the method described in this paper was simple and effective to prevent the active materials from exfoliation in practical use.

3.6 Permselectivity

The crosslinked and quaternized membrane was directly employed for the membrane potential (Em) measurement without using other supporting layers such as a non-woven PET mat. Moreover, it was sustained for a week without dissolution. It indicated that the strength of this membrane was strong enough to be a self-supporting microfiltration membrane. KCl, KNO3 and K2SO4 were selected to evaluate the permeability of anions at 25°C, and the results are listed in Table 3. The permeabilities of NO3, Cl and SO42− were 94, 91 and 87%, indicating a good permselectivity of membrane. Obviously, the smaller radius of hydrated anions, the faster anions migrate in solution.

Table 3:

The permeability of different ions.

IonsNO3ClSO42−
Permeability (P)94%91%87%

4 Conclusions

In this paper, a new approach was proposed to fabricate a self-supporting microfiltration membrane, for the purpose of improving the uniformity of active group distribution in a membrane, the hydrophilicity of the membrane and the effectiveness of grafted active materials as well as the mechanical properties. Copolymer of poly N,N-dimethylaminoethyl methacrylate (DMAEMA)-co-2-hydroxyethyl methacrylate (HEMA) (HEMA/DMAEMA=4/1) was prepared by using AIBN as initiator in DMF. In preliminary experiments, DMF was selected as the electrospinning solvent, and the concentration of total copolymer should be above 40 wt% regardless to the composition of HEMA and DMAEMA. The electrospinning optimal parameters were determined by orthogonal experiments. It was confirmed that the concentration of total copolymer was the decisive factor to determine the uniformity of microfibers. The optimal electrospinning conditions were: the concentration, 42 wt%; voltage, 10 kV; flow rate, 1.0 ml/h; distance, 12 cm. Under these conditions, the uniform diameter of microfibers was about 1200 nm with a deviation of 0.05. The mat was crosslinked at 60°C with the formaldehyde vapor. The water sorption decreased from 75.7% to 30.4% as the crosslinking time increased from 20 h to 32 h. The robust mat with the high tensile strength of 4.62 MPa and 50% elongation at the break was obtained at 24 h. After quaternizing the amino groups in the membrane with CH3I vapor at room temperature for a week, the ion permeability of the mat was measured without any supporting material. The mat was sustainable in salt solution for a week without any dissolution and biofouling. This result indicated that the mechanical strength was strong enough for the mat to be used as a self-supporting microfiltration membrane. The permselectvities of NO3, Cl, SO42− were 94, 91 and 87%, respectively.

Acknowledgments

This work was supported by the Natural Science Foundation of China (NSFC No.51541302), and was financially assisted by the Nanjing Science and Technology Committee (Platform No 2014-030002) and the Priority Academic Program Development of Jiangsu Higher Education Institutions (PAPD). All the experiments and data analysis were conducted by Mr. Yadong Yang.

References

1. Subramanian S, Seeram R. New directions in microfiltration applications – are the microfibers right materials as membranes in desalination? Desalination 2013;308:198–208.10.1016/j.desal.2012.08.014Search in Google Scholar

2. Greiner A, Wendorff JH. Electrospinning: a fascinating method for the preparation of ultrathin fibers. Angew Chem Int Ed. 2007;46:5670–703.10.1002/anie.200604646Search in Google Scholar PubMed

3. Ahmed FE, Lalia BS, Hashaikeh R. A review on electrospinning for membrane fabrication: Challenges and applications. Desalination 2015;356:15–30.10.1016/j.desal.2014.09.033Search in Google Scholar

4. Agarwal S, Jiang S. Microfibers and electrospinning. In: Kobayashi S Müllen K, editors. Encyclopedia of polymeric nanomaterials, Berlin Heidelberg: Springer, 2015:1323–37. ch. 370.10.1007/978-3-642-29648-2_370Search in Google Scholar

5. Wang X, Chen X, Yoon K, Fang D, Hsiao BS, Chu B. High flux filtration medium based on microfibrous substrate with hydrophilic nanocomposite coating. Environ Sci Technol. 2005;39:7684–91.10.1021/es050512jSearch in Google Scholar PubMed

6. Wang X, Fang D, Yoon K, Hsiao BS, Chu B. High performance ultrafiltration composite membranes based on poly(vinyl alcohol) hydrogel coating on crosslinked microfibrous poly(vinyl alcohol) scaffold. J Membr Sci. 2006;278:261–8.10.1016/j.memsci.2005.11.009Search in Google Scholar

7. Yoon K, Kim K, Wang X, Fang D, Hsiao BS, Chu B. High flux ultrafiltration membranes based on electrospun microfibrous PAN scaffolds and chitosan coating. Polymer 2006;47:2434–41.10.1016/j.polymer.2006.01.042Search in Google Scholar

8. Sata T, Yamaguchi T, Matsusaki K. Effect of hydrophobicity of ion exchange groups of anion exchange membranes on permselectivity between two anions. J Phys Chem. 1995;99(34):12875–82.10.1021/j100034a028Search in Google Scholar

9. Satinderpal K, Sundarrajan S, Gopal R, Ramakrishna S. Formation and characterization of polyamide composite electrospun microfibrous membranes for salt separation. J. Appl Polym Sci. 2012;124:E205–15.10.1002/app.36375Search in Google Scholar

10. Satinderpal K, Rajendrakumar Barhate S, Sundarrajan S, Matsuura T, Ramakrishna S. Hot pressing of electrospun membrane composite and its influence on separation performance on thin film composite nanofiltration membrane. Desalination 2011;279:201–9.10.1016/j.desal.2011.06.009Search in Google Scholar

11. Prince JA, Singh G, Rana D, Matsuura T, Anbharasi V, Shanmugasundaram TS. Preparation and characterization of highly hydrophobic poly(vinylidene fluoride)-clay nanocomposite nanofiber membranes (PVDF-clay NNMs) for desalination using direct contact membrane distillation. J Membr Sci. 2012;397–398:80–6.10.1016/j.memsci.2012.01.012Search in Google Scholar

12. Dos Santos L, Rose S, Sel O, Marechal M, Perrot H, Laberty-Robert C. Electrospinning a versatile tool for the designing hybrid proton conductive membrane. J Membrane Sci. 2016;513:12–9.10.1016/j.memsci.2016.04.002Search in Google Scholar

13. Wang G, Pan C, Wang L, Dong Q, Yu C, Zhao Z, Qiu J. Activated carbon nanofiber webs made by electrospinning for capacitive deionization. Electrochim Acta. 2012;69:65–70.10.1016/j.electacta.2012.02.066Search in Google Scholar

14. Jiang S, Hou H, Agarwal S, Greiner A. Polyimide Nanofibers by “Green” electrospinning via aqueous solution for filtration applications. ACS Sustainable Chem Eng. 2016;4:4797–804.10.1021/acssuschemeng.6b01031Search in Google Scholar

15. Liu CX, Zhang DR, He Y, Zhao XS, Bai RB. Modification of membrane surface for anti-biofouling performance: Effect of anti-adhesion and anti-bacteria approaches. J Membrane Sci. 2010;346:121–30.10.1016/j.memsci.2009.09.028Search in Google Scholar

16. Ong CS, Goh PS, Lau WJ, Misdan N, Ismail AF. Nanomaterials for biofouling and scaling mitigation of thin film composite membrane: a review. Desalination 2016;393:2–15.10.1016/j.desal.2016.01.007Search in Google Scholar

17. Ni H-M, Ma G-H, Nagai M, Omi S. Effects of ethyl acetate on the soap-free emulsion polymerization of 4-vinylpyridine and styrene. I. aspects of the mechanism. J Appl Polym Sci. 2001;82:2679–91.10.1002/app.2121Search in Google Scholar

18. Ni H-M, Ma G-H, Nagai M, Omi S. Novel method of preparation of a charged mosaic membrane by using dipole-like microspheres. II. Preparation of dumbbell/egg-like microspheres. J Appl Polym Sci. 2001;80:2002–17.10.1002/app.1298Search in Google Scholar

19. Chen Y-L, Cui Y-M, Jia Y-S, Zhan K, Zhang H, Chen G-X, Yang Y-D, Wu M, Ni H-M. Preparation of charged mosaic (CM) membrane of sodium polystyrene sulfonate (PNaSS) and poly(4-vinyl pyridine) (P4VP) by conjugate electrospinning. J Appl Polym Sci. 2014;131:40716.10.1002/app.40716Search in Google Scholar

20. Teoh RL, Guice KB, Loo Y-L. Atom transfer radical copolymerization of hydroxyethyl methacrylate and dimethylaminoethyl methacrylate in polar solvents. Macromolecules 2006;39:8609–15.10.1021/ma061650bSearch in Google Scholar

21. Martin-Gomis L, Cuervo-Rodriguez R, Fernandez-Monreal MC, Madruga EL, Fernandez-Garcia M. Copolymerization reactivity ratios and glass transition temperature of copolymers based dimethyl amino ethyl methacrylate and two structural hydroxyl-functional acrylate isomers. J Polym Sci Part A: Polym Chem. 2003;41:2659–66.10.1002/pola.10811Search in Google Scholar

22. Jiang S, Hou H, Greiner A, Agarwal S. Tough and transparent nylon-6 electrospun Nanofiber reinforced melamine-formaldehyde composites. ACS Appl Mater Interf. 2012;4:2597–603.10.1021/am300286mSearch in Google Scholar PubMed

23. He Y, Han D, Chen J, Ding Y, Jiang S, Hu C, Chen S, Hou H. Highly strong and highly tough electrospun polyimide/polyimide composite microfibers from binary blend of polyamic acids. RSC Adv. 2014;4:59936–42.10.1039/C4RA10075ASearch in Google Scholar

24. Jiang S, Duan G, Zussman E, Greiner A, Agarwal S. Highly flexible and tough concentric triaxial polystyrene fibers. ACS Appl Mater Interf. 2014;6:5918–23.10.1021/am500837sSearch in Google Scholar PubMed

Received: 2016-8-2
Accepted: 2016-9-25
Published Online: 2016-10-18
Published in Print: 2017-3-1

©2017 Walter de Gruyter GmbH, Berlin/Boston

This article is distributed under the terms of the Creative Commons Attribution Non-Commercial License, which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.

Downloaded on 10.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/epoly-2016-0207/html
Scroll to top button