Ki-Tae Bang‡
,
Hyung-Seok Lim‡,
Seong-Jin Park and
Kyung-Do Suh*
Department of Chemical Engineering, College of Engineering, Hanyang University, Seoul, 133-791, Republic of Korea. E-mail: kdsuh@hanyang.ac.kr
First published on 1st July 2015
This paper presents a novel, facile method for fabricating pH-responsive inorganic/organic composite microspheres with hollow structures in the absence of a step for the removal of the core. Using polyelectrolyte (hydrogel) hollow microspheres without a need for further calcination and chemical etching, minimally cross-linked poly(methacrylic acid/ethylene glycol dimethacrylate/3-(trimethoxysilyl) propylmethacrylate), poly(MAA/EGDMA/TMSPM) [pMET] microspheres were prepared by a distillation–precipitation method. Once the pMET microspheres disperse in 2-propanol, the hollow structure is clearly observed and can be maintained more rigidly in a dry state after amorphous TiO2 (a-TiO2) is incorporated into the shell of a microsphere by a sol–gel method. The a-TiO2-incorporated pH-responsive pMET composite [pMET/TiO2] hollow microspheres were tested as a photocatalyst in acidic and neutral conditions. The photocatalytic performance of the hollow pMET/TiO2 composite microcapsules under neutral condition was better than that under acidic conditions due to their large active surface and strong adsorption ability against methylene blue (MB).
In this paper, we present a facile template-free method of preparing pH-responsive poly(methacrylic acid/ethylene glycol dimethacrylate/3-(trimethoxysilyl)propylmethacrylate), poly(MAA/EGDMA/TMSPM) [pMET] microspheres with a hollow structure without injecting additional molecules like CTA+, and subsequently hollow pMET microspheres decorated with amorphous TiO2 (a-TiO2) nanoparticles using a sol–gel process. The hollow pMET/a-TiO2 microspheres can capture the cationic organic pollutants in an aqueous solution under alkaline and neutral conditions because the polyelectrolyte body could have a strong negative charge. These composite microcapsules exhibit strong dye adsorption ability. The captured organic dyes are decomposed efficiently by photocatalysis of a-TiO2 nanoparticles embedded in the polyelectrolyte body.
Fig. 1a–c present the results of SEM and Raman and FT-IR spectroscopy of the pMET microspheres with low crosslinking density. The pMET microspheres exhibited a spherical shape even in the dry state while the poly(MAA/EGDMA) [pME] microspheres in the absence of TMSPM were obtained as a film in the dry state, as shown in Fig. S1.† Fig. 1b and c show Raman spectrum of pMET microspheres and FT-IR spectra of the pME and pMET microspheres. The Raman spectrum shows the characteristic band of the Si–OCH3 group observed at 2934 and 2993 cm−1, implying that the pMET microspheres have some forms of the Si–OCH3 group as a functional site for the proceeding sol–gel reaction.18 From the FT-IR spectra, the pMET microspheres show the absorption peak corresponding to the Si–O–Si stretching vibration characteristics at 1063 cm−1 instead of the Si–OCH3 stretching vibration at 1083 cm−1, while the pME microspheres did not have corresponding peak for either Si–O–Si or Si–OCH3. These results indicated that the pMET microspheres not only have crosslinking networks with Si–O–Si bonding caused by a sol–gel reaction during the polymerization process, but also the Si–OCH3 group. Fig. 2 shows CLSM images of the pMET microspheres dispersed in aqueous solution and 2-propanol, respectively. The CLSM image of the pMET microspheres dispersed in aqueous solution exhibits a crosslinking density gradient from the particle center trending outward, as shown in Fig. 2a. Since the pMET microspheres have a low crosslinking density and the Si–O–Si bond exhibits secondary crosslinking, a partial hydrophobic interaction may occur. When the particles dispersed in aqueous solution were moved into 2-propanol, the internal cavity was generated from the center of the particle. Fig. 2b shows a CLSM image of the hollow-structured pMET microspheres dispersed in 2-propanol. In order to verify the generation of the hollow structure, we carried out an additional experiment. When the dried pMET microspheres were dispersed in water and 2-propanol, the particles dispersed in 2-propanol could not swell, whereas the particles dispersed in water were swollen, as shown in Fig. S2.† herefore, the internal cavity was generated by increase in the hydrophobicity of the polymer matrix.
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Fig. 1 (a) SEM image and (b) Raman spectrum of the pMET microspheres, and (c) FT-IR spectra of the pMET and pME microspheres. |
Amorphous TiO2 nanoparticles were incorporated into the hollow pMET microspheres in 2-propanol using titanium isopropoxide. After being stirred for 40 h, the supernatant was removed by centrifugation with ethanol and a large amount of water was added into the reactor with precipitates. The sol–gel reaction occurred in the polymer phase as well as on the surface of the particle. The light-yellow-colored powders were obtained by centrifugation and dried at room temperature. Fig. S3† shows XRD patterns of the p(MET) and p(MET)/a-TiO2 composite microspheres and a-TiO2 nanoparticles. XRD pattern of the p(MET)/a-TiO2 composite microspheres exhibited only two broad peaks around 16° and 32° corresponding to the poly(MAA/EGDMA) microspheres. According to the XRD pattern of a-TiO2 nanoparticles that synthesized by sol–gel reaction without polymer templates, TiO2 nanoparticles formed in the polymer phase display low crystallinity, as shown in Fig. S3.† Fig. 3 shows SEM, FIB-SEM, TEM, EDX maps, and HR-TEM images of the hollow pMET/a-TiO2 composite microcapsules. The hollow pMET/a-TiO2 composite microcapsules have a rough surface due to the a-TiO2 nanoparticles coated on the surface of pMET microspheres, as shown in Fig. 3a. The focused ion beam (FIB) SEM and TEM images of the hollow pMET/a-TiO2 composite microcapsules indicate that the composite microcapsules have a large internal cavity even in a dry state, as shown in Fig. 3b and c.
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Fig. 3 (a) SEM, (b) FIB-SEM, (c) TEM, ((d): carbon, (e): titanium) HR-TEM based EDX maps of the hollow pMET/a-TiO2 composite microcapsules, and the corresponding (f) HR-TEM image. |
Fig. 3d and e show EDX maps of carbon and titanium elements in the hollow pMET/a-TiO2 composite microcapsules, and we found that the Ti atoms were diffused into the polymer phase during mechanical stirring in 2-propanol. In addition, the a-TiO2 nanoparticles were aggregated on the surface of the microcapsules because the residual titanium ions reacted with water outside of the polymer microspheres. We matched the HR-TEM image with EDX maps and drew a domain of a-TiO2 in the composite hollow microcapsules, as shown in Fig. 3f. Fig. 4a shows TGA curves of the a-TiO2 nanoparticles, the hollow pMET/a-TiO2 and the pMET microspheres. A weight loss of about 30% was observed during heating to 900 °C in the TGA curve of the a-TiO2 nanoparticles, as shown in Fig. 4a (red line). The hollow pMET/a-TiO2 composite microcapsules exhibited a weight loss in the range of 350–450 °C, attributed to the thermal degradation of the polymer chains (black line), and the residual mass refers to the amount of inorganic materials consisting of SiO2 and TiO2 in composite microcapsules at above 450 °C. The TGA curve of the pure pMET microspheres shows the residual mass to be 8.11% at 450 °C (blue line), which might consist of SiO2 formed during polymerization. These TGA curves demonstrated that the pMET microspheres have an inorganic segment, and the a-TiO2 nanoparticles were well incorporated into the hollow pMET/a-TiO2 microspheres. We also examined the number of elements in composite microcapsules through EDX analysis, as shown in Fig. 4b. Fig. 5a shows OM images of the hollow pMET/a-TiO2 composite microcapsules dispersed in aqueous solution at different pHs (2, 7 and 11). When the pH value of the aqueous solution containing particles changed from 2 to 11, the particle size increased from 2.1 to 5.3 μm. A plot of the diameter variations of the pMET and hollow pMET/a-TiO2 composite microcapsules according to pH is shown in Fig. 5b. The lower swelling degree of the hollow pMET/a-TiO2 composite microcapsules is attributed to the amorphous TiO2 shell coated on the surface of the polymer particle as well as 3D networks of TiO2 and SiO2 formed in the polymer phase.
In the photo-degradation system, the degree of adsorption for organic pollutants on the surface of photocatalysts is very important because the oxidization and reduction of the organic molecules by electron and hole transfers involve interfacial reactions. The concept of photocatalytic degradation in this work is related to two factors; (1) the electrostatic attraction between negative-charged polymer microcapsules and positive-charged organic pollutants and (2) the interfacial area between photocatalysts and organic molecules, as in Fig. S4.† The hollow pMET/a-TiO2 composite microcapsules are swollen in aqueous solution, as shown above because the hollow polymer chains have negative electrostatic repulsion due to ionization of the carboxylic acid groups. Since methylene blue (MB) has been used as a representative positive-charged dye in aqueous solution, we chose MB to use as an organic pollutant in this experiment.
The test of adsorption ability for the hollow pMET/a-TiO2 composite microcapsules was completed in acidic, neutral and alkali aqueous solutions containing the same concentration of MB. Fig. 6a shows that a small amount of MB (about 4%) was adsorbed into pMET/a-TiO2 microcapsules under acidic condition (pH 2), while most MB molecules were adsorbed into pMET/a-TiO2 microcapsules under neutral (pH 7) and alkali (pH 11) conditions after magnetic stirring for 10 min. The digital photographs also show that the MB molecules were fully adsorbed in the hollow pMET/a-TiO2 composite microcapsules under neutral and alkali aqueous solutions, as shown in Fig. 6b and c. In order to obtain the exact photocatalytic ability of the hollow pMET/a-TiO2 microspheres, we regulated three conditions. (i) Temperature: the degradation of MB molecules is significantly affected by heat, as shown in Fig. S5a.† Based on the experimental results, we fixed the temperature in the system to 20 °C; (ii) pH condition: MB concentration in aqueous solution depends on the pH value of the system, as shown in Fig. S5b.† To minimize the losses of natural degradation for MB, we tested only acidic and neutral conditions; (iii) stirred during UV irradiation: most photocatalytic experiments were examined with mechanical stirring because the dispersion of photocatalyst powders is important to react with organic pollutants. Our materials are based on the hydrogel having a great affinity with water molecules, which are well floated in aqueous solution without precipitation during mechanical stirring. The photocatalytic ability of the hollow pMET/a-TiO2 composite microcapsules was evaluated in acidic and neutral aqueous solutions by exposing MB molecules under UV irradiation. The changes in the MB concentration were analyzed as a function of irradiation time, as shown in Fig. 5c. The degradation rate of the hollow pMET/a-TiO2 microcapsules under the neutral condition is much faster than the sample under the acidic condition. Although the TiO2 nanoparticles incorporated into the hollow polymer microcapsules are amorphous, it is obvious that the MB dye can react with a-TiO2 under UV irradiation. The photocatalytic efficiency of hollow pMET/a-TiO2 microcapsules under acidic and neutral conditions can be obtained from Fig. 5c. After UV irradiation for 180 min, the degradation ratio can reach over 69.74% in the neutral medium, compared with only 26.9% in the acidic medium. Even if the photocatalytic efficiency obtained by subtracting the losses of natural degradation for the hollow pMET/a-TiO2 microcapsules under the neutral condition was about 35% after UV irradiation for 180 min (Fig. S5b†), the photocatalytic efficiency under the neutral condition was still higher than that under acidic condition. For acidic condition, a small amount (about 4%, Fig. S6a†) of MB molecules can be adsorbed on the surface of a-TiO2 nanoparticles coated on the hydrogel microspheres. However, most MB molecules cannot be diffused into the composite microcapsules because of the reduced negative charge of the composite microcapsules. Therefore, the photocatalytic reaction occurs at the interface between a-TiO2 nanoparticles coated on the surface of the hollow pMET/a-TiO2 microcapsules and MB molecules dispersed in the medium. As shown in Fig. S6b,† on the other hand, in the case of neutral condition, the MB molecules are degraded inside of the swollen microcapsules as well as on their surface because most MB molecules are incorporated into the swollen gels by strong electrostatic attraction between negatively-charged gels and the MB dye together with the adsorption on the surface of a-TiO2 nanoparticles. Consequently, this better photocatalytic efficiency is attributed to the large surface of reactive materials and the strong adsorption ability of the hollow pMET/a-TiO2 microcapsules under neutral condition.
Footnotes |
† Electronic supplementary information (ESI) available: SEM images of poly(MAA/EGDMA) microspheres; OM images of poly(MAA/EGDMA) microspheres dispersed in 2-propanol and water; XRD pattern of pMET/a-TiO2 composite microcapsules; additional schematic illustration; thermodegradation and photodegradation of MB without photocatalysts; FT-IR spectra of all samples. See DOI: 10.1039/c5ra06231d |
‡ These authors contributed equally to this work. |
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