Yonghong Ni*a,
Hangsong Zhenga,
Nannan Xianga,
Kefeng Yuana and
Jianming Hongb
aCollege of Chemistry and Materials Science, Key Laboratory of Functional Molecular Solids of Education Ministry, Anhui Key Laboratory of Functional Molecular Solids, Anhui Laboratory of Molecule-Based Materials, Anhui Normal University, 1 Beijing Eastern Road, Wuhu, 241000, PR China. E-mail: niyh@mail.ahnu.edu.cn; Fax: +86-553-3869303
bCenters of Modern Analysis, Nanjing University, Nanjing, 210093, PR China
First published on 9th December 2014
Coral-like BaTiO3 nanostructures were successfully synthesized via a simple hydrothermal route at 150 °C for 15 h employing BaCl2, tetrabutyl titanate [(C4H9O)4Ti] and NaOH as reactants without the assistance of any surfactant or template. The phase of the as-obtained BaTiO3 was characterized by X-ray powder diffraction (XRD). Energy dispersive spectrometry (EDS), scanning electron microscopy (SEM) and (high-resolution) transmission electron microscopy (TEM/HRTEM) were employed for the composition and morphology analyses of the final product. Some factors influencing the formation of the coral-like BaTiO3 nanostructures were investigated, including the amount of NaOH, the barium ion source, and the reaction temperature and time. Experiments showed that the as-prepared coral-like BaTiO3 nanostructures presented good photocatalytic activity for the degradation of methyl orange (MO) dye under the irradiation of artificial sunlight. It was found that the photocatalytic activity of the coral-like BaTiO3 nanostructures could be affected by the pH value of the system.
As one of the prominent ferroelectric and piezoelectric materials, perovskite-type BaTiO3 is mainly applied in multilayer capacitors, nonvolatile memories, thermistors, transducers, and electro-optical devices due to its large dielectric constant and nonlinear optical coefficient.4–6 Recently, however, some titanate-based materials including BaTiO3 were found to bear good photocatalytic activities.7–11 Obviously, these are useful exploration for environmental treatments.
Many studies have discovered that the properties of a material are usually dependent on its shape and/or size. Thus, it has become a goal to prepare BaTiO3 nanostructures with a certain morphology. However, the conventional method to synthesize BaTiO3 is the solid-phase reaction between BaCO3 and TiO2 at a high temperature, ca. 1100 °C. The morphology and size of BaTiO3 cannot be easily controlled by the solid-phase route; thus, only irregular particles with micrometer scales are often obtained. Unlike the solid-phase process, the morphology- and size-controlled synthesis of a material can be easily realized in wet chemical routes through simply adjusting experimental parameters. To date, employing various solution-phase approaches, many BaTiO3 micro/nanostructures with different morphologies and sizes have been successfully obtained including core–shell particles, plate-like particles, nanoporous structures, nanotubes, tetragonal and dendritic structures.12–17 In 2008, Maxim et al. hydrothermally synthesized BaTiO3 micro/nanostructures by the reaction of titanate layered nanotubes and barium hydroxide.17 Simultaneously, they investigated the influence of the reaction temperature and time on the shape of the final product, and found that dendritic BaTiO3 microstructures could be generated at 200 °C for 24 h or 110 °C for 114 h. However, the performance of the product was ignored. Recently, Lee and coworkers prepared cubic BaTiO3 nanoparticles through a hydrothermal route at 100–180 °C for 24–72 h, employing P25-TiO2 and Ba(OH)2 as the reactants. Simultaneously, the UV light-assisted photocatalytic activity of the as-obtained BaTiO3 nanoparticles was investigated.18
Distinctly, the hydrothermal synthesis of BaTiO3 micro/nano-structures has been reported in literature.17,18 However, high reaction temperatures or/and long reaction times were often needed. Simultaneously, some specific reactants were used. In the present work, we designed a mild hydrothermal route to successfully prepare coral-like BaTiO3 nanostructures. BaCl2, tetrabutyl titanate and NaOH were used as reactants. The reactions were carried out at 150 °C for 15 h, without the assistance of any surfactant or template. Compared with previous reports,17,18 a lower temperature, shorter time, and/or common reactants were employed. At the same time, the photocatalytic performance of the BaTiO3 nanostructures under the illumination of an artificial sunlight was studied. More importantly, considering the practical applications, the influence of pH on the photocatalytic performance of BaTiO3 was also investigated.
To investigate the influence of the amount of NaOH, the above preparation process was repeated under the presence of 0, 12 and 24 mmol NaOH.
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Fig. 1 (a) The XRD pattern, (c) FTIR spectrum and (d) TG analysis of the product prepared by the current hydrothermal route; (b) EDS analyses of the product before and after heat-treatment. |
In the present simple hydrothermal system, the formation of BaTiO3 should be obtained by following two reactions:
(C4H9O)4Ti + 4H2O = Ti(OH)4 + 4C4H9OH | (1) |
BaCl2 + Ti(OH)4 + 2NaOH = BaTiO3 + 2NaCl + 3H2O | (2) |
The produced BaTiO3 nanostructures could adsorb the n-butyl alcohol generated in eqn (1) owing to the high surface energy of the nanoparticles, which resulted in the high C content. To prove the abovementioned speculation, the FTIR spectrum of the final product was obtained. As shown in Fig. 1c, the broad and strong band centered at 3435 cm−1 is assigned to the O–H stretching vibration of the interlayer water molecules and the H-bound OH group. Another peak observed at 1634 cm−1 is assigned to the bending vibration of water molecules.19 A weak peak at 2925 cm−1 belongs to the stretching vibration of –CH2– group. The two broad characteristic bands below 700 cm−1 are assigned to the Ti–O vibration modes. Another characteristic band of the crystalline barium titanate phase is observed at 1444 cm−1.20 Fig. 1d shows the TGA curve of the obtained product. Although the total weight loss is only 8% in the range from room temperature to 600 °C, two weight-loss regions can be observed. The first weight loss located at 100–200 °C should be ascribed to the desorption of physically adsorbed water on the surfaces of the coral-like BaTiO3 nanostructures.10 The second one is found in the range of 200–470 °C, which should be appearing due to the loss of surface organic molecules and chemically bonded hydroxyl groups.10 Here, EDS technology was again employed for the component analysis of the calcined product. As shown in the upper curve of Fig. 1b, the C content in the product dramatically decreases. This fact proves that the high C content in the uncalcined product was due to the adsorption of organic compounds.
The morphology of the as-obtained BaTiO3 was observed by SEM and TEM techniques. Fig. 2a shows a representative low-magnification SEM image of the product. Coral-like nanostructures can be observed easily. Further enlargement shows that the ends of the coral-like nanostructures present dendritic structures (see Fig. 2b), which were confirmed by the TEM observations. As shown in Fig. 2c, the products are solid dendrites with diameters of 100–200 nm. An HRTEM image of the product is depicted in Fig. 2d. The clear lattice fringes are visible. The distance between neighbouring planes is measured to be 0.397 nm, which is very close to 0.4003 nm of the (010) plane of cubic BaTiO3 (JCPDS no. 86-1569). Furthermore, the SAED pattern shown in Fig. 2d confirms the good crystallinity of the coral-like BaTiO3 nanostructures.
Furthermore, the Ba2+ ion source could also affect the formation of the coral-like BaTiO3 nanostructures. Fig. 4a and b shows the typical SEM images of the products prepared from the systems containing Ba(CH3COO)2 and Ba(NO3)2, respectively, under the same experimental conditions. Obviously, aggregated nanoparticles and rods were generated when Ba(CH3COO)2 was used as the Ba2+ ion source instead of BaCl2 (see Fig. 4a). However, when Ba(NO3)2 was selected as the Ba2+ ion source, coral-like nanostructures were still the main product in addition to some big grains (see Fig. 4b). The abovementioned facts demonstrate that the counter anion also plays an important role in the formation of BaTiO3 with various shapes. Generally, CH3COO− anions have a stronger coordinative ability to some metal ions than the Cl− and NO3− anions. Thus, it is possible that the BaTiO3 nuclei were surrounded by CH3COO− anions, which was unfavorable to the oriented growth of the BaTiO3 crystals. As a result, no coral-like nanostructures were formed. Due to the weak interaction to BaTiO3, however, Cl− or NO3− ions could only occupy small amounts of active sites, and the BaTiO3 nuclei could grow oriented along the directions unoccupied by Cl− or NO3− ions. Thus, coral-like nanostructures were finally obtained.
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Fig. 4 SEM images of the products prepared under the same experimental conditions with different Ba2+ ion sources: (a) Ba(CH3COO)2 and (b) Ba(NO3)2. |
Further investigations showed that coral-like BaTiO3 nanostructures were always obtained in the proper temperature and time ranges. Namely, the reaction temperature and time hardly affected the morphology of the final product in the present experimental conditions. Based on the abovementioned experimental facts, in the present simple hydrothermal system, the possible formation mechanism of coral-like BaTiO3 nanostructures can be described as follows: with the production of BaTiO3, the saturation of the system increased. BaTiO3 gradually nucleated and grew. Because some active sites of the BaTiO3 nuclei were occupied by Cl− ions, BaTiO3 nanocrystals grew oriented along the directions unoccupied by Cl− ions. Finally, coral-like BaTiO3 nanostructures were formed.
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Fig. 5 UV-vis diffuse reflectance spectra of BaTiO3 nanostructures prepared from the systems containing various amount of NaOH. The inset is the plot of (ahν)2 ∼ hν. |
Based on the consideration of practical applications, sunlight should be the most ideal irradiation source. In our experiments, a 500 W of Xe lamp without a filter was used as the illumination source. Thus, an artificial sunlight containing UV light was obtained. To investigate the photocatalytic performance of the as-obtained BaTiO3 nanostructures, certain amounts of BaTiO3 nanostructures were dispersed in a methyl orange (MO) solution of 10 mg L−1. Fig. 6a shows the absorption spectra of the MO aqueous solutions irradiated by the artificial sunlight source for various durations in the presence of 30 mg of coral-like BaTiO3 nanostructures. The characteristic peak of MO gradually decreases with the extension of the irradiation time. After 90 min, the MO solution is almost colorless (see the insert in Fig. 6a). Under the irradiation of the light, generally, photogenerated electrons and holes can be formed in a photocatalyst.23
Photocatalyst + hv → photocatalyst + e− + h+ | (3) |
Then, the holes react with water molecules or OH− to produce ˙OH radicals with strong oxidative activity.24
h+ + H2O → ˙OH + H+ | (4) |
Thus, organic molecules such as MO dyes adsorbed on the surface of the photocatalyst are finally oxidized by ˙OH radicals. The abovementioned degradation process should also be applicable in our work.
Furthermore, it was found that the catalytic efficiency of the photocatalyst could be affected by its amount. As seen from Fig. 6b, when no catalyst was used, ∼40% MO was degraded within 90 min under the same light source. After 20 mg BaTiO3 was employed, ∼75% MO was degraded under the same experimental conditions. When the amount of BaTiO3 was increased to 30 mg, ∼92% MO was removed from the aqueous solution. Upon further increasing the amount of BaTiO3 to 40 mg, however, only ∼71% MO was degraded. Namely, the degradation efficiency of the catalyst decreased. It was believed that the solid catalyst could prevent the utilization of the light, especially at high concentrations.25 Thus, excess BaTiO3 could not promote the catalytic efficiency.
In practical applications, wastewater is often acidic or alkaline. Therefore, it is very significant to investigate the influence of the pH of the system on the catalytic efficiency of the catalyst. Fig. 7 depicts the correlation curves between the degradation efficiency of the catalyst to the MO dye and the pH of the system in the presence of 30 mg BaTiO3 under the same experimental conditions. One can find that the degradation efficiency of the catalyst first decreased with the increase of the pH value from 1 to 7, and then increased with the pH from 7 to 13. Under the neutral system, the catalyst presents the lowest catalytic efficiency. Moreover, the degradation efficiencies are higher under acidic conditions than those under basic conditions (see the inset in Fig. 7). Lee et al. considered that the surfaces of photocatalysts with a negative charge easily adsorbed cationic species, while anionic ones were readily adsorbed on the surfaces of positively charged photocatalysts.18 In the present solution with 10 mg L−1 MO, the pH of the system was ∼5. When the pH was adjusted by HCl to a lower value, the surfaces of the coral-like BaTiO3 nanostructures became positive, which was made available for adsorbing more negatively charged MO molecules on their surfaces. Markedly, this facilitated the degradation of the MO dye. In addition, Ba2+ ions could be leached from BaTiO3 nanocrystals in neutral aqueous solution and the leaching rate became faster with the pH decrease of the system.26 Here, TiO2 was produced on the surface of the BaTiO3 nanocrystals according to the following reaction:20,26
BaTiO3(s) + 2H+(aq) = Ba2+(aq) + TiO2(s) + H2O(aq) | (5) |
Thus, the catalytic efficiency of the product was improved in the acidic system. Different from the acidic system, however, more hydroxyl radicals with high oxidation capability were generated at the higher pH values, which also promoted the degradation of MO dye.27–29
Moreover, we also investigated the influence of the morphology of the catalyst on the photocatalytic performance. As shown in Fig. 8, when the BaTiO3 particles prepared under the presence of 12 mmol or 24 mmol NaOH were used as the catalyst, respectively, the degradation efficiencies were in turn 50% and 40%, respectively, within 90 min, which are far lower than 92% of the coral-like nanostructures. Obviously, the abovementioned degradation efficiency change should be related to the morphology of the final product. Generally, the morphology change of a catalyst can cause its surface area to change. Accordingly, its adsorptive capacity will be also different. Fig. 9 shows the BET surface areas and BJH adsorption average pore diameters of the final products prepared from the systems containing 6 and 12 mmol NaOH. The BET surface areas and BJH adsorption average pore diameters are 74.1 m2 g−1 and 7.7 nm, and 17.1 m2 g−1 and 9.4 nm, respectively. Markedly, the surface area of the product decreased with the increase of NaOH amount in the initial system. As a result, the adsorptive capacity of the catalyst decreased, and accordingly the degradation efficiency decreased. Moreover, as mentioned previously, the content of BaCO3 increased in the final product with the increase of NaOH amount. This is another possible reason to cause the photocatalytic capacity decrease of the catalyst in addition to the influence of the morphology.
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Fig. 8 The comparison of the photocatalytic efficiency of the catalyst in the presence of 30 mg BaTiO3 nanostructures with various shapes prepared from systems containing 6, 12 and 24 mmol of NaOH. |
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Fig. 9 BET surface areas and pore size distribution of the BaTiO3 nanostructures prepared under the same conditions with different NaOH concentrations: (a) 6 mmol and (b) 12 mmol. |
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