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Pore structure of macroporous polymers using PS/ silica composite particles as Pickering stabilizers Shuhua Tu, Chenxu Zhu, Lingyun Zhang, Haitao Wang, and Qiangguo Du Langmuir, Just Accepted Manuscript • DOI: 10.1021/acs.langmuir.6b03285 • Publication Date (Web): 18 Nov 2016 Downloaded from http://pubs.acs.org on November 20, 2016
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Pore structure of macroporous polymers using PS/silica composite particles as Pickering stabilizers †
†
Shuhua Tu, Chenxu Zhu, Lingyun Zhang, Haitao Wang,* and Qiangguo Du
State Key Laboratory of Molecular Engineering of Polymers, Collaborative Innovation Center of Polymers and Polymer Composite Materials, Department of Macromolecular Science, Fudan University, Shanghai 200433, P. R. China
ABSTRACT A novel approach for preparation of interconnected macroporous polymers with controllable pore structure was reported. The method was based on polymerization of a water-in-oil (w/o) Pickering high internal phase emulsion (HIPE) stabilized by polystyrene/silica composite particles. The composite Pickering stabilizers were facilely obtained by mixing positively charged polystyrene (PS) microspheres and negatively charged silica nanoparticles, and their amphiphilicity could be delicately tailored by varying the ratio of PS and silica. The droplet size of Pickering HIPEs was characterized by an optical microscope. The pore structure of polymer foams was observed by a scanning electron microscope (SEM). The interconnectivity of macroporous polymers was evaluated upon their gas permeability, which was greatly improved after etching PS microspheres included in Pickering stabilizers with tetrahydrofuran. As a result, fine tailoring of pore structure of polymer foams could be realized by simply tuning the ratio of PS to silica particles in the composite stabilizer.
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INTRODUCTION Porous polymers have been widely used in many fields such as catalysts,1,2 separation,3,4 storage,5,6 tissue engineering scaffolds,7-9 and sound and heat insulation10-12 owning to their low density and high porosity. Various applications of porous polymers are heavily relied on their pore structures. Although many methods have been reported on fabrication of porous polymers,13-16 emulsion templates attract great attentions due to the facile tailoring of pore size and size distribution of resulting polymer materials. With a minimum internal phase volume fraction of 74%, high internal phase emulsions (HIPEs) are often used as templates to produce high porosity polymers.17-22 Conventional
HIPEs
are
commonly
stabilized
by
surfactants
including
cetyltrimethylammonium bromide (CTAB), sorbitan monooleate (Span 80), and amphiphilic polymers, which are toxic and not environmental friendly. A large amount of surfactant is required to produce stable HIPEs (5~50 wt %23 relative to the continuous phase), which gives rise to the additional producing cost. Moreover, macroporous polymers prepared from HIPEs generally show undesirable mechanical strength.24 Thus these poly-HIPEs are obviously restricted for further applications, especially in biomedical materials. Instead of molecular surfactants, solid particles with appropriate surface property such as silica,25-28 titania29,30 and iron oxide nanoparticles31-33 can also stabilize HIPEs, which are often referred to as Pickering HIPEs. However, pristine solid particles are often too hydrophilic or too hydrophobic to effectively stabilize HIPEs, and thus they still need to be modified using certain surfactants34,35, thus making the modification process more tedious.36,37 Many efforts have been devoted to obtaining stable Pickering HIPEs by using surfactant-free stabilizers. Colloidal celluloses and various cellulose derivatives were found to be capable of stabilizing simple oil-in-water systems.38 Some other colloidal particles, including chitosan nanocrystals,39,40 protein particles,41,42 fat crystals and wax microparticles43,44, could also successfully stabilize HIPEs. However, these reports mostly focus on the stability of Pickering HIPEs rather than the pore structures of poly-HIPEs, which have rarely been explored. 2
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Polymer foams with interconnected pores have been reported in the systems where HIPE templates are stabilized by surfactants.24,45-47 In the case of Pickering HIPEs, though a small quantity of pores are interconnected by pore throats formed during polymerization process, control over the interconnectivity in poly-Pickering HIPEs still remains challenging.24 Thus, applications of such macroporous polymers in the fields of adsorption, filtration and tissue engineering scaffolds are restrained. There have been only several reports about Pickering HIPEs concentrating on the formation of open-cell structure so far. Interconnected porous polymers are formed by introducing the molecular surfactants,45,46 or drawing the solid particles from the interface through monomer-particle reaction.48 Recently, we prepared polymer foams with open pore structures by extracting the thin monomer layer between two adjacent emulsion droplets using the flocculation with lipophilic core.26 It’s also an effective method to form pore throats by using the monomer with high polymerization shrinkage.25 In this work, a surfactant-free composite Pickering stabilizer is facilely prepared only by mixing positively charged polystyrene (PS) microspheres and negatively charged silica nanoparticles. The wettability of the composite stabilizer is easily tailored by varying the ratio of PS microspheres and silica nanoparticles. Stable water-in-oil HIPEs with controllable droplet size can be produced when PS/silica composite particles are used as Pickering stabilizers. Open-cell macroporous polymers are achieved after polymerization of Pickering HIPEs with relatively high PS microsphere concentration and their interconnectivity is further improved by etching with tetrahydrofuran.
EXPERIMENTAL SECTION Materials. Silica hydrosol (28 nm, 40.0%) was supplied by Fujian Sanbang Chemical Co. (China). Tetrahydrofuran (THF, 99%) was purchased from Sinopharm Chemical Reagent
Co.
(China).
Styrene
(St,
99%),
divinylbenzene
(DVB,
80%),
[2-(methacryloyloxy) ethyl] trimethylammonium chloride (MATMAC, 75%), 3
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2,2'-azobis
(2-methylpropionamidine)
dihydrochloride
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(AIBA,
99%)
and
2,2'-azobisisobutyronitrile (AIBN, 99%) were provided by Aladdin Chemistry Co., Ltd. Styrene and divinylbenzene were purified by distillation under vacuum and AIBN was recrystallized with ethanol prior to use. Deionized water was used throughout the experiments. Synthesis of PS/silica composite Pickering stabilizers. PS microspheres were prepared by a soap-free emulsion polymerization method. In a typical procedure, AIBA (0.05 g) was dissolved in water (107.5 g) in a 250 mL three-necked flask equipped with magnetic stirring and nitrogen protection, and then St (9.375 g) and MATMAC (0.277 g) were added. After heating at 70 oC for 12 h, PS microspheres dispersed in water were obtained. Crosslinked PS microspheres were prepared in a similar route, only instead of 9.375 g St a mixture of 8.438 g St and 0.937g DVB was used. PS/silica composite particles were fabricated by dropping silica hydrosol into PS microspheres aqueous dispersion according to the recipe listed in Table 1. Then the mixture was sonicated for 10 min before preparing Pickering HIPEs.
Table 1. Recipes for the preparation of PS/silica composite Pickering stabilizers sample
silica particles (wt %)a
PS microspheres (wt %)a
1 2 3 4 5 6 7 8
0.20 0.25 0.30 0.35 0.40 0.45 0.50 0.55
0.80 0.75 0.70 0.65 0.60 0.55 0.50 0.45
a
With respect to aqueous phase.
Preparation of Pickering HIPEs. Pickering emulsions were prepared using PS/silica composite particles as the 4
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stabilizers. The oil phase (1.25 mL) consisting of 80 vol% St and 20 vol% DVB was added to 5mL aqueous phase containing PS/silica composite Pickering stabilizer. The mixture was then vigorously emulsified with Vortex-BE1 at 500 rpm for 10 min to form Pickering HIPEs. Preparation of Poly-Pickering HIPEs. Initiator AIBN (1.0 wt %) was dissolved in the oil phase prior to the preparation of Pickering HIPEs when the samples would undergo the polymerization. The Pickering HIPEs were transferred into centrifuge tubes, sealed and placed in a 65 oC oil bath for 24 h. The poly-HIPEs were then obtained after drying in a convection oven at 60 oC for 48 h. Characterization. Both hydrodynamic diameter and zeta potential of silica nanoparticles and PS colloidal particles were measured on a Malvern ZS90. The hydrodynamic diameter was measured in a PS cell at 25 °C. The zeta potential was measured in a universal dip cell in a PS cuvette for potential measurements at 25 °C under pH 7. The concentration of the suspension was 0.1 wt %. Photographs of Pickering HIPEs, PS colloidal particles and silica hydrosol were taken by a Sony Xperia Z5P digital camera. The morphology of the Pickering emulsion droplets was observed by an EV5680 optical microscope. The type of Pickering emulsions (w/o or o/w) was assessed by the drop test.49 The pore structure of the macroporous polymers was observed by a Tescan 5136MM scanning electron microscope (SEM). The morphology of PS microspheres was observed by a Zeiss Ultra 55 field-emission scanning electron microscope (FE-SEM). All samples were placed onto carbon-coated lacy substrates and the polymer samples were sputtered with gold before observation. The mean pore size of the poly-Pickering HIPEs was obtained by averaging size of at least 100 pores estimated from SEM images. The permeability of the poly-Pickering HIPE was characterized by measuring the flow rates of nitrogen passing through the sample at 5000 Pa. The macroporous polymers were cut into cylinders with a length of 10 mm and a diameter of 14 mm. 5
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Each sample was measured three times.
RESULTS AND DISCUSSION Preparation of PS/silica composite Pickering stabilizers Silica hydrosol is normally too hydrophilic to stabilize Pickering emulsions, and thus surfactants are used to tailor its amphiphilicity.25,50,51 Polystyrene (PS) microspheres obtained via a soap-free emulsion polymerization are also very hydrophilic due to the charges on the surface. The charge neutralization of negatively charged silica nanoparticles and positively charged PS microspheres hereby is developed as a new way to endow the composite particles with appropriate amphiphilicity for the subsequent stabilization of Pickering HIPEs. The average diameters of PS microspheres and silica nanoparticles are 103 nm and 57 nm, respectively (see Figure 1). The white flocculation is clearly observed when silica hydrosols are dropped into PS microspheres aqueous dispersion, indicating the strong electrostatic attraction between polymer and inorganic particles (see Figure 2). The zeta potentials of PS particles and silica nanoparticles are measured to be +49.7 ± 0.6 and -20.0 ± 0.8 mV, respectively. Obviously, zeta potential of PS particles decreases gradually as increasing content of silica particles and approaches neutral when the concentration of silica reaches 60 wt % (see Figure 3). Therefore, the extremely hydrophilic surface of PS particles can be suitably hydrophobized via this facile and efficient route for the subsequent preparation of stable Pickering HIPEs. It is worth noting that no other molecular surfactants are involved, indicating an environmental friendly modification process.
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Figure 1. Size distribution of (a) silica nanoparticles and (b) PS microspheres in water.
Figure 2. Photographs of (a) PS microspheres aqueous dispersion, (b) silica hydrosol, and (c) PS/silica composite particles (sample 2, Table 1).
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Figure 3. Zeta potentials of PS/silica composite particles with different composition of silica nanoparticles in a constant particle concentration of 0.1 wt %.
Preparation of HIPEs Figure 4 shows the emulsions stabilized by the composite stabilizers with different ratios of silica particles to PS microspheres. With a low silica/PS ratio of 1:4, the PS/silica composite particles are still too hydrophilic to stabilize water-in-oil HIPE due to the strong positive charges on PS surface (see Figure 4a). Pickering HIPEs are prepared successfully when silica/PS ratio in PS/silica composite particles increases (Figure 4b and c), although they flow down slowly when the centrifuge tubes are inverted. With further increasing the silica/PS ratio, HIPEs with high viscosity and stability are obtained (Figure 4d-g). However, when the silica/PS ratio increases as high as 11:9, no stable HIPEs are formed probably due to the extreme flocculation of silica particles and PS microspheres (Figure 4h). During this neutralization process, PS surface is believed to be covered by silica particles in steps as increasing silica amount. The naked surface of PS microspheres renders the composite particles 8
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lipophilic while the packed silica particles promise a good affinity toward water. With a proper flocculation extent, the PS/silica composites have optimal stabilization effort for HIPEs. But when extremely large aggregations of silica and PS are produced, the zeta potential approaches minus, meaning that the surfaces of PS microspheres are fully covered by hydrophilic silica particles. It has been reported that solid particles with extreme hydrophilicity or hydrophobicity are unable to stabilize Pickering emulsions.52-54 Meanwhile, the gravity of such large aggregates cannot be neglected anymore at oil/water interface, which is bad for stabilization of Pickering emulsions. Therefore, PS/silica composite particles with too high silica content (sample 8, Table 1) are not able to stabilize HIPEs (Figure 4h).
Figure 4. Photographs of w/o Pickering HIPEs stabilized by composite particles with different weight ratios of silica particles to PS microspheres: (a) 1:4, (b) 1:3, (c) 3:7, (d) 7:13, (e) 2:3, (f) 9:11, (g) 1:1, and (h) 11:9 (samples 1-8, Table 1).
Pickering HIPEs stabilized by PS/silica composite particles were observed by an EV5680 optical microscope. As shown in Figure 5a-d, the droplet size of Pickering HIPEs decreases with increasing silica/PS ratio in PS/silica composite particles from 1:3 to 2:3. Notably, further increment of silica/PS ratio to 9:11 or more (1:1) leads to a larger droplet size of formed HIPEs, instead (see Figure 5e and f). We attribute the size difference of emulsion droplets to the different stabilization effect of composite Pickering stabilizers. As demonstrated above, weak flocculation of oppositely charged PS microspheres and silica nanoparticles can vary the PS surface from extremely 9
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hydrophilic to amphiphilic due to charge neutralization, which facilitates the effective stabilization of HIPEs. However, over flocculated composite particles sacrifice their surface amphiphilicity due to full coverage of PS surface by hydrophilic silica nanoparticles, indicating a poor stabilization for water-in-oil HIPEs. In short, the size of Pickering HIPEs could be adjusted effectively by varying the ratio of silica to PS in the composite particles.
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Figure 5. Optical microscopy images of Pickering HIPEs stabilized by composite particles with different weight ratios of silica particles to PS microspheres: (a) 1:3, (b) 3:7, (c) 7:13, (d) 2:3, (e) 9:11, and (f) 1:1 (samples 2-7, Table 1). Preparation of poly-Pickering HIPEs After polymerization of Pickering HIPE templates, porous polymers are obtained, as shown in Figure 6. The pore size of macroporous polymers are measured by averaging size of at least 100 pores estimated from SEM images and plotted in Figure 7. It decreases first, and then increases with the content of silica in the composite stabilizer. The pore size of poly-Pickering HIPEs is in a good agreement with the droplet size of the original emulsions, indicating that the coalescence of adjacent droplets is suppressed during polymerization procedure. Interestingly, some pore throats are clearly observed, as shown in Figure 6a-d. To our knowledge, polymerization of Pickering HIPEs mainly produces closed-cell pores. Although some pores are interconnected by pore throats, the interconnectivity is still out of control because the solid particles surround the emulsion droplets acting as barriers.55-57 Considering that PS/silica composites play as Pickering stabilizers of HIPEs in our system, PS microspheres are swollen by St before polymerization. Thus, the monomer layer between two emulsion droplets becomes thinner initially and the pore throats are then produced due to the split on the weak walls when polymerization shrinkage occurs.
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Figure 6. SEM images of poly-Pickering HIPEs stabilized by composite particles with different weight ratios of silica particles to PS microspheres: (a) 1:3, (b) 3:7, (c) 7:13, 12
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(d) 2:3, (e) 9:11, and (f) 1:1 (samples 2-7, Table 1).
Figure 7. Pore size of poly-Pickering HIPEs stabilized by composite particles with different concentration of silica nanoparticles in PS/silica composite stabilizer (samples 2-7, Table1). In order to verify the formation mechanism of pore throats, crosslinked PS microspheres which are hardly swollen by monomer, were prepared in comparison with uncrosslinked ones. As seen in Figure 8, there is no obvious difference in appearance between uncrosslinked and crosslinked PS microsphere powders. Besides, the size and the morphology of the microspheres are almost the same (see Figure 9). However, the solution of uncrosslinked PS microspheres in monomer becomes transparent and the viscosity increases a lot, while a turbid dispersion is obtained when crosslinked PS particles are mixed with monomer. This result again confirms that uncrosslinked PS microspheres are easily swollen by St, but crosslinked ones are not. Crosslinked PS colloidal particles are also mixed with silica hydrosol as the 13
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recipe of sample 2 in Table 1 to prepare the Pickering stabilizer and the subsequent Pickering HIPEs. In our case, the size of uncrosslinked PS microspheres after swelling is larger than that of crosslinked ones which are hardly swollen by monomer. It has already been demonstrated that larger Pickering stabilizer often stabilizes larger emulsion droplets, and vice versa.58 Therefore, smaller droplet size of HIPEs as well as smaller pore size of poly-HIPEs is anticipated when substituting crosslinked PS/silica composite particles for uncrosslinked PS/silica composite particles as Pickering stabilizer (see Figure 10a and 10b). Moreover, as shown in Figure 10b few open throats are observed, which is significantly different from the pore structure in the previous case (see Figure 6a). We think one possible reason is that the oil layer between two water droplets is too thick to be torn up during polymerization because crosslinked PS microspheres cannot extract monomer from the oil phase. Gas permeability test (Figure 11) confirms that the interconnectivity of poly-Pickering HIPEs is greatly improved by using uncrosslinked PS/silica composite stabilizers.
Figure 8 Images of (a) uncrosslinked and (b) crosslinked PS microspheres in dried state (left) and after dispersed in St (right).
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Figure 9. FE-SEM images of (a) uncrosslinked and (b) crosslinked PS microspheres.
Figure 10. (a) Optical microscopy image of Pickering HIPEs and SEM images of poly-Pickering HIPEs stabilized by crosslinked PS/silica composite particles (b) before and (c) after etching with THF (sample 2, Table 1). 15
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Figure 11. Gas permeability of poly-Pickering HIPEs stabilized by PS/silica composite particles containing (a) uncrosslinked or (b) crosslinked PS microspheres (sample 2, Table 1).
The results above have demonstrated that polymer foams with interconnected pore structures can be achieved when uncrosslinked PS/silica composite particles are used as Pickering stabilizers. Since THF is a good solvent for dissolving uncrosslinked PS, which are immobilized initially at the monomer/water interface and then at the pore wall after polymerization, more and larger pore throats would be expected when exposing the poly-Pickering HIPEs to THF. Figure 12 shows morphology of poly-Pickering HIPEs after treatment with THF. It’s clearly seen that the samples have many larger pore throats compared with those prior to THF treatment as shown in Figure 6. The amount of pore throats decreases with lowering content of PS microspheres in the composite particles. While etching the poly-Pickering HIPE stabilized by crosslinked PS/silica composite particles with THF, there was no obvious difference before (Figure 10b) and after (Figure 10c) THF treatment, 16
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indicating that the crosslinked PS microspheres are hardly washed up. The interconnectivity of polymer foams before and after THF etching is also characterized by the gas permeability test and the result is plotted in Figure 13. It is clear that the permeability of macroporous polymers is enhanced obviously after THF treatment, especially for those using the composite stabilizer with high PS content. This is in good agreement with SEM images. In a word, both the gas permeability and SEM results suggest that the interconnectivity of macroporous polymers can be facilely tailored by simply varying the weight ratio of uncrosslinked PS in the composite particles upon treatment with THF.
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Figure 12. SEM images of poly-Pickering HIPEs stabilized by composite particles with different weight ratios of silica particles to PS microspheres after etching with THF: (a) 1:3, (b) 3:7, (c) 7:13, (d) 2:3, (e) 9:11, and (f) 1:1 (samples 2-7, Table 1).
Figure 13. Gas permeability of poly-Pickering HIPEs stabilized by uncrosslinked PS/silica composite particles with different PS/silica weight ratios before and after THF treatment (samples 2-7, Table 1). 18
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CONCLUSIONS Environmental friendly PS/silica composites are facilely prepared by mixing positively charged PS colloidal particles and negatively charged silica nanoparticles as Pickering stabilizer to produce stable w/o HIPEs without any other surfactants. The amphiphilicity of the composite stabilizer is tailored by varying the ratio of PS to silica, and thus the droplet size of Pickering HIPES as well as the pore size of poly-Pickering HIPEs is tuned conveniently. Dominantly over other Pickering stabilizer, PS/silica composite particles immobilized on the oil/water interface can extract monomer from the continuous phase, thus thinning the monomer layer between adjacent water droplets and finally producing open-cell structure due to the split of week interface during polymerization. The interconnectivity of polymer foams can be further improved by etching with THF, especially for the samples with high PS content in composite stabilizer. This kind of polymer/silica composite Pickering stabilizer probably opens a new gateway for tailoring the pore structure, especially interconnectivity of polymer foams, meeting the requirements of various applications.
ASSOCIATED CONTENT AUTHOR INFORMATION Corresponding Author *E-mail:
[email protected] Author Contributions †
These authors contributed equally to this work.
Notes The authors declare no competing financial interests. ACKNOWLEDGMENTS This work was financially supported by the National Natural Science Foundation of China (NSFC) (No. 51373038).
REFERENCES (1) Chen, Z.; Zhao, C.; Ju, E.; Ji, H.; Ren, J.; Binks, B. P.; Qu, X. Design of 19
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Table of Contents Graphic and Synopsis
Pore structure of macroporous polymers using PS/silica composite particles as Pickering stabilizers
Shuhua Tu,† Chenxu Zhu,† Lingyun Zhang, Haitao Wang,* and Qiangguo Du
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