Open Access Article
Mingxing Chen,
Changfa Xiao
*,
Chun Wang and
Hailiang Liu
State Key Laboratory of Separation Membranes and Membrane Processes, School of Material Science and Engineering, Tianjin Polytechnic University, Tianjin 300387, China. Web: xiaochangfa@163.com Tel: +86 022-83955299
First published on 7th April 2017
Novel braid-reinforced (BR) and thermostable poly(m-phenylene isophthalamide) (PMIA) hollow fiber membranes comprising reinforced braids and a separation layer were prepared by a dry–wet spinning process for the first time. The effects of PMIA concentration and the braid composition on the structure and performance of the BR PMIA hollow fiber membranes were investigated. Field emission scanning electron microscopy (FESEM) was used to observe the morphologies of the BR PMIA hollow fiber membranes. An increase in PMIA concentration resulted in an increase of the protein rejection rate and a decrease in the pure water flux. The higher flux recovery rate indicated that the BR PMIA membranes had excellent antifouling property compared to commercial PVDF membranes. In the BR PMIA membranes existed favorable interfacial bonding between the separation layer and the reinforced braids as the tensile strength of the BR PMIA membranes exceeded 170 MPa. Moreover, when the operating temperature was increased from 25 °C to 90 °C, the water flux increased more than two-fold with stable ink solution rejection, which showed an excellent thermal stability.
Some studies have been done to promote the mechanical properties of hollow fiber membranes,8–11 such as the reinforced membrane, which displays good tensile strength and a self-supporting capability. However, a problem still remains that the separation layer could be easily peeled from the reinforced matrix of this kind of hollow fiber membrane, which was termed as a heterogeneous reinforced (HTR) hollow fiber membrane, as the separation layer and reinforced matrix are incompatible. It is desirable that the homogeneous reinforced (HMR) hollow fiber membrane uses the same material between the reinforced matrix and the separation layer to enhance the interfacial bonding. Fan12,13 prepared HMR cellulose acetate (CA) hollow fiber membranes by coating CA solution onto the CA hollow tubular braids. Liu14,15 and Zhang7,16 fabricated reinforced polyvinyl chloride (PVC) and reinforced polyvinylidene fluoride (PVDF) hollow fiber membranes, respectively, and found that the HMR membranes had a more favorable interfacial bonding between the reinforced matrix and the separation layer compared with HTR membranes.
The thermally stable membranes have recently gained significant attention for their advantages, such as flux enhancement, heat recovery, high temperature cleaning, and pasteurization, while commercial membranes can only be applied below the temperature of 50 °C.17 Although ceramic membranes still have undeniable advantages in terms of thermal stability, the high cost and difficult manufacturing process remain critical problems limiting their wide use. Thus it is valuable to develop polymeric membranes with outstanding thermal stability. Some research has been done to develop polymeric membranes with excellent thermal stability, such as polybenzimidazole (PBI),18,19 poly(phthalazine ether sulfone ketone) (PPESK),20,21 sulfonated poly(phthalazinone ether sulfone) (SPPES),22 poly(phthalazione ether nitrile ketone) (PPENK),23 poly(phthalazinone ether amide) (PPEA),24 and poly(pyromellitic dianhydride-co-4,4-oxydianiline) (PMDA/ODA PI).25 However, the poorer hydrophilic property and higher price of these materials limit their application.
Poly(m-phenylene isophthalamide) (PMIA) is one of the most important aromatic polyamides and has been used widely in nanofibers for its high thermal stability combined with excellent mechanical properties.26–31 The chemical structure formula and thermodynamics performance of PMIA are shown in Fig. 1, S1 and S2.† The aramid groups and hydrogen bond network in PMIA contribute to its outstanding thermal stability, hydrophilic property, and mechanical properties. Studies focused on the application of PMIA membranes in water treatment have achieved a certain level of development in the last few years. Ren32 and Huang33 successfully fabricated a PMIA nanofiltration membrane via a phase inversion method, which demonstrated high performance when it was used in removing chromium(VI) from chromium-containing wastewater and in applications of dye purification and desalination. Wang34 fabricated a PMIA hollow fiber nanofiltration membrane by dry–wet spinning technology. The effects of non-solvent additives on the morphology and separation performance were studied. The results indicated that it is possible to fabricate PMIA hollow fiber NF membranes with desired structures and separation performances by adding proper concentrations of LiCl, acetone, and PVP in the doping solution. In another study by Wang,35 a PMIA hollow fiber membrane was used for the removal of perfluorooctane sulfonate from water. The result suggested that the PMIA hollow fiber membrane had potential for applications in the removal of perfluorooctane sulfonate from water. Yang36 prepared a novel PMIA/GO composite nanofiltration membrane via a phase inversion method. The novel PMIA/GO composite nanofiltration membrane showed higher water flux and an excellent antifouling performance due to the addition of GO, which showed its potential for application in water treatment. Lin37 fabricated a PMIA ultrafiltration membrane via a phase inversion method. In this study, the PMIA membrane was found to break through the trade-off between selectivity and permeability. However, to the best of our knowledge, reinforced PMIA hollow fiber membranes and their thermal stability have never been studied before.
In the present study, the braid-reinforced (BR) PMIA hollow fiber membranes were prepared by a dry–wet spinning process and their properties were evaluated by analyzing their morphology, permeability, mechanical property, antifouling property, and thermal stability. The effects of polymer concentration and the composition of the reinforced braids on the structure and performance of the BR PMIA hollow fiber membranes are discussed herein.
000 Da) was purchased from SRO Aramid Co. Ltd. (Huaian, China). Poly(ethylene glycol) (PEG, Mw = 2000), N,N-dimethylacetamide (DMAc), calcium chloride(CaCl2), and lithium chloride(LiCl) were purchased from Tianjin Kermel Chemical Reagent Co. Ltd. (Tianjin, China). Polyvinylpyrrolidone (PVP, Analytical Reagent, K30, Mw = 30
000) were bought from BASF Chemical Industrial Co. Ltd. (Ludwigshafen, Germany). Bovine serum albumin (BSA, Mw = 68
000) was purchased from Beijing Newprobe Bioscience Co., Ltd. (Beijing, China). The commercial PVDF membrane was provided by OriginWater Technology Co. Ltd. (Beijing China). PMIA filament (PMIA fiber) was purchased from Yantai Tayho Advanced Materials Co. Ltd. (Yantai, China). PET filament (PET fiber) was purchased from Rong Sheng Chemical Fiber Co. Ltd. (Hangzhou, China). The parameters of the PMIA and PET filaments are shown in Table S1.†
| Membrane ID | PMIA (wt%) | PVP (wt%) | PEG (wt%) | CaCl2 (wt%) | LiCl (wt%) | DMAc (wt%) | Braids compositions PMIA/PET |
|---|---|---|---|---|---|---|---|
| PMIA5 | 5 | 2 | 8 | 3.5 | 2.5 | 79 | 2/0 |
| PMIA8 | 8 | 2 | 8 | 3.5 | 2.5 | 76 | 2/0 |
| PMIA10 | 10 | 2 | 8 | 3.5 | 2.5 | 74 | 2/0 |
| PMIA15 | 15 | 2 | 8 | 3.5 | 2.5 | 69 | 2/0(M1), 1/1(M2), 0/2(M3) |
The water contact angle of the membrane was measured using a contact angle goniometer (Kruss DSA-100, Germany). The average contact angle was calculated with five water contact angles at different locations in order to get a reliable value.
The surface charge of the membranes was determined by measurement of the zeta potentials with the streaming potential method. The measurements were carried out at a temperature of 25 °C in KCl solution (0.001 M, 500 mL) with the pH ranging from 11 to 4 with an electrokinetic analyzer (SurPASS, Anton Paar, Austria).
The pore size and distribution of the membranes were measured by a mercury porosimeter (AutoPore IV 9500, Micromeritics, USA). The samples were all freeze-dried for more than 24 h before testing.
The pure water flux (PWF) of the membranes was measured using a cross-flow filtration system (Fig. S5†) at an outside pressure of 0.1 MPa, and then calculated using eqn (1):
![]() | (1) |
The BSA rejection and antifouling tests were measured with 1 g L−1 BSA aqueous solution at 0.1 MPa. The flux of the BSA solution was recorded as J1. The rejection was calculated by eqn (2):
![]() | (2) |
After the BSA fouled membranes were washed with unionized water, the pure water flux of the cleaned membranes (J2) was measured again. The flux recovery ratio (FRR) was calculated by eqn (3):38,39
![]() | (3) |
To further analyze the antifouling properties of the membranes in detail, several ratios, including the total flux decline ratio (DRt), the reversible decline ratio (DRr), and the irreversible decline ratio (DRir), were defined and calculated as follows:39,40
![]() | (4) |
![]() | (5) |
![]() | (6) |
The mechanical property of the hollow fiber membranes was evaluated by using a universal material testing machine (5969, INSTRON Corporation, America) with a loading velocity of 5 mm min−1 and an initial length of 30 mm. Every sample was tested more than five times.
The bursting strength is the pressure required to rupture a membrane. The bursting strength of the hollow fiber membranes was measured using the apparatus shown in Fig. S6,† comprising a dead-end filtration system under the condition of inside pressure.
In order to evaluate the thermal stability of the membrane, the ink solution was used as the filtration solution. During the test, the operation temperature was raised from 25 °C to 90 °C, while the water flux and the rejection were tested, respectively. The particle distribution and standard concentration absorbance curve of the ink solution are shown in Fig. S7 and S8.† The commercial PVDF membrane and PMIA hollow fiber membrane without braid reinforcement were tested as a control under the same conditions.
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| Fig. 4 The morphologies of the BR PMIA hollow fiber membranes: (a) cross-section, (b) partial enlargement of the cross-section, (c) outer surface of: (1) PMIA5, (2) PMIA8, (3) PMIA10, (4) PMIA15. | ||
The outer surface morphologies of the BR PMIA hollow fiber membrane are shown in Fig. 4c, where it can be seen that the outer surface became denser and smoother as the PMIA concentration increased in the doping solutions. This is beneficial to improving the rejection and antifouling ability of the membrane, though it would lead to a lower flux.
The cross-sectional morphologies of the BR PMIA hollow fiber membrane with various braid compositions are shown in Fig. 5. The reinforced braid of M1, M2, and M3 were prepared with the PMIA filament, PMIA/PET filament, and PET filament, respectively. As shown in Fig. 5, the separation layer of M1 was tightly bonded with the reinforced braid as they were homogeneous, which ensures a good compatibility. M3, on the other hand, had a poor interfacial boding state as the PET reinforced braid and separation layer were heterogeneous, which means a poor compatibility. For M2, whose reinforced braid was prepared by the PMIA/PET filament, both phenomena existed and it could be seen that the separation layer tightly bonded with the PMIA fibers, while at the same time it had a poor interfacial bonding state with the PET fibers. Moreover, the M1 membranes, which belonged to HMR hollow fiber membranes, did not exhibit a dense region formed by the swelling of the PMIA fibers like the other HMR hollow fiber membranes,13 which was beneficial to the permeability of the membranes. This was because it was a little bit difficult for DMAc in the doping solution to swell the PMIA fiber in such a short time. That was also the reason why we added LiCl and CaCl2 to the DMAc solution when we prepared the doping solution.46 So we considered that the effort of the hybrid braid combined with the PET and PMIA fibers may have no significance in the present work compared to others,12 though it would reduce the cost of the BR PMIA hollow fiber membranes. The reinforced braid prepared with the PMIA filament was thus employed in our following study. Some characterizations of the BR PMIA hollow fiber membranes are shown in Table S2.†
| Membrane ID | PMIA5 | PMIA8 | PMIA10 | PMIA15 | PVDF |
|---|---|---|---|---|---|
| Contact angle (°) | 50.4 ± 2.58 | 53.8 ± 2.25 | 52.9 ± 3.46 | 54.8 ± 2.51 | 75 ± 3.26 |
| Membrane ID | PMIA5 | PMIA8 | PMIA10 | PMIA15 |
|---|---|---|---|---|
| Average pore diameter (nm) | 620.3 | 417.7 | 180.2 | 148.2 |
The effect of PMIA concentration on PWF is shown in Fig. 8. As shown in Fig. 8, the PWF decreased from 296.85 L m−2 h−1 for PMIA5 to 75.78 L m−2 h−1 for PMIA15 when the concentration of PMIA is increased in the doping solution. This was because the higher PMIA concentration leads to a smaller pore size and denser surface, which results in a decrease in membrane permeability. Fig. 8 also indicated that the PWF decline gradually slowed down with the increase in PMIA concentration. This was because the higher PMIA concentration promoted the resistance to the compaction of the porous membranes.48
The effect of PMIA concentration on separation of BSA solution is shown in Fig. 9. As shown in Fig. 9, the rejection increased with the test time increasing, which was because the pollutant deposition leads to a cake layer on the membrane surface with the test time, finally reaching 77.3%, 88.5%, 92.7%, and 97.9% for PMIA5, PMIA8, PMIA10, and PMIA15, respectively. The rejection of PMIA5 was lower than the others due to the big pore size, as shown in Fig. 7. A high PMIA concentration in the doping solution led to a denser skin layer and smaller pore size distribution, as shown in Fig. 4 and 7. Thus, the BSA rejection increased from 77.3% to 97.9% when the PMIA concentration was increased.
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| Fig. 10 Rejection and flux recovery of the BR PMIA hollow fiber membranes in the separation process of a skim milk solution: (a) rejection, (b) the pure water flux before and after filtration. | ||
In order to further analyze the antifouling properties of BR PMIA, a simple fouling experiment with BSA solution was studied. The mean average pore size of the commercial PVDF membrane was 0.1 μm, which was close to PMIA15 (0.148 μm). Thus, both the PMIA15 and the commercial PVDF membrane were tested, respectively. The flux recovery was tested after the fouled membranes washed with deionized water. The flux recovery ratio (FRR) and total flux decline ratio (DRt) were the characteristic parameters related to the membrane antifouling property. The higher value of FRR and lower value of DRt indicated a better antifouling property of the membrane. The results are shown in Fig. 11. As shown in Fig. 11, the FRR values of PMIA15 and the commercial PVDF membrane were 96.68% and 74.23%, respectively. Simultaneously, the DRt values of PMIA15 and the commercial PVDF membrane were 35.39% and 65.11%. These results indicated that PMIA15 had better antifouling properties for protein than commercial PVDF membrane. The DRr and DRir values of PMIA15 were 32.07% and 3.32%, while those of the commercial PVDF membrane were 39.34% and 25.77%. The deposition and irreversible adsorption of BSA aggregates onto the membrane surface induced an irreversible fouling, whereas the deposition and weak interaction of BSA aggregates to the membrane surface induced a reversible fouling.39 The strong electronegativity and excellent hydrophilicity hindered the irreversible adsorption and deposition of BSA aggregates to the membrane surface and induced more deposition and a weak interaction of BSA aggregates, which enhanced the antifouling property of the membranes. As mentioned above, the PMIA membrane had a stronger electronegativity and excellent hydrophilicity compared to the PVDF membrane, so that the PMIA15 membrane had a better antifouling property than the commercial PVDF membrane.
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| Fig. 11 Time-dependent permeate flux of PMIA15 membranes and commercial PVDF membranes (a), and the summary of the corresponding FRR, DRt, DRr, DRir values (b) during BSA solution filtration. | ||
| Sample | Initial modulus (MPa) | Tensile strength (MPa) | Breaking elongation (%) | Bursting strength (MPa) |
|---|---|---|---|---|
| PMIA braid | 88.1 ± 0.81 | 193.87 ± 1.02 | 78.96 ± 0.55 | |
| PMIA5 | 312.5 ± 8.24 | 178.76 ± 2.35 | 68.2 ± 4.15 | 0.367 ± 0.029 |
| PMIA8 | 372.2 ± 6.48 | 173.15 ± 3.21 | 63.42 ± 2.79 | 0.467 ± 0.029 |
| PMIA10 | 510.1 ± 9.66 | 172.66 ± 4.65 | 63.5 ± 3.09 | 0.583 ± 0.029 |
| PMIA15 | 924.4 ± 11.1 | 179.15 ± 3.73 | 63.2 ± 3.89 | 0.983 ± 0.029 |
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| Fig. 12 The flux and rejection of the BR PMIA hollow fiber membranes at different temperatures for: (a) the BR PMIA membranes, (b) the commercial PVDF membranes. | ||
In order to further analyze the thermal stability of the BR PMIA hollow fiber membranes, the PMIA hollow fiber membranes fabricated via a phase invasion method without braid reinforcement were applied to compare the thermal stability with the BR PMIA hollow fiber membranes. The compositions of the doping solution of the PMIA hollow fiber membrane were identical with that of PMIA15. As shown in Fig. 14, the flux of the PMIA hollow fiber membranes increased while the rejection remained stable when the operation temperature ranged from 25 °C to 90 °C. This indicated that the PMIA hollow fiber membranes also had a better thermal stability. However, the flux of the PMIA hollow fiber membranes was lower than that of the BR PMIA hollow fiber membranes. As shown in Fig. S9,† both the BR PMIA hollow fiber membranes and PMIA hollow fiber membranes had a dense outer layer, while the BR PMIA hollow fiber membranes had a relatively porous inner layer compared with the PMIA hollow fiber membranes. This should result in a lower mass transfer resistance of BR PMIA hollow fiber membranes; therefore, the BR PMIA hollow fiber membranes had a superior flux than the PMIA hollow fiber membranes. As a consequence, the BR PMIA hollow fiber membranes may be a better choice compared with PMIA hollow fiber membranes.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra01171g |
| This journal is © The Royal Society of Chemistry 2017 |