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Journal of Nanomaterials
Volume 2013 (2013), Article ID 294020, 7 pages
Surfactant-Free Solvothermal Method for Synthesis of Mesoporous Nanocrystalline TiO2 Microspheres with Tailored Pore Size
College of Chemical Engineering, Shenyang University of Chemical Technology, Shenyang 110142, China
Received 24 January 2013; Accepted 9 March 2013
Academic Editor: Guo Gao
Copyright © 2013 Yajing Zhang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
TiO2 mesoporous microspheres self-assembled from nanoparticles were synthesized by a surfactant-free solvothermal route. The TiO2 precursors were fabricated by tetrabutyl titanate, glacial acetic acid, and urea in the ethanol solution at 140°C for 20 h, and TiO2 mesoporous microspheres were obtained by a postcalcination at temperatures of 450°C for promoting TiO2 crystallization and the removal of residual organics. The phase structure, morphology, and pore nature were characterized by XRD, SEM, and nitrogen adsorption-desorption measurements. The as-prepared TiO2 microspheres are in anatase phase, with 2-3 μm in diameter, and narrow pore distribution range is 3-4 nm. The adjustments of the synthetic parameters lead to the formation of the mesoporous TiO2 microspheres with tuned pore size distributions and morphology.
The existence of a close relationship between specific morphologies and unique properties in nanomaterials has ignited much attention to the synthesis of novel nanostructures for a broad domain of applications in the past decade . Due to its large surface area, networked pore distribution, and unique band structure, mesoporous TiO2 has attracted explosive attention for photocatalytic applications, such as water splitting, water and air purification, antibacterial materials and sterilization [2, 3]. A lot of chemical synthetic methods have been developed for fabricating the TiO2 nanomaterials, including sol-gel , hydrolysis , precipitation , and hydrothermal methods [7, 8]. Hydrothermal method has been widely used for preparing mesoporous TiO2 owing to the controllable morphology and porous structure as well as the high crystallization degree of the product . It is found that phase selection (rutile, anatase, or brookite), particle shape and size, and crystal orientation with specific lattice plane are controllable depending on synthetic conditions [10–12]. Nevertheless, few reports focus on the effect of synthetic conditions on the pore size distribution. Most synthesis processes use template for the growth of anisotropic nanocrystals. Templates used include hard template (porous silica, alumina, or latex spheres, etc.) and soft template (triblock copolymer or surfactants) [13–15]. However, after synthesis, the template has to be removed from the sample to make the pores accessible. This can be achieved by thermal treatment (calcination) or solvents extraction . In most cases, TiO2 mesoporous materials are calcined; the thermal treatment processes frequently lead to the partial or total collapse of the porous structure during the template removal process and thus result in the decrease of the surface area . In addition, some template cannot be completely removed by either calcination or solvent extraction because it tightly bound to the materials. Therefore, developing approaches without template and surfactant to overcome these limitations are highly demanded. Moreover, during the process of use, TiO2 nanomaterials are subjected to the difficulties in handling and additional cost for recycling process; thus micro- and submicrometer scaled materials are often preferred in the large-scale production .
Here, mesoporous TiO2 microspheres self-assembled from nanoparticles have been fabricated by a surfactant-free, convenient, and low-cost solvothermal method, which can conquer the issues above-mentioned. In addition, the diameters size, pore volume, BET surface areas, and the pore size distributions can also be tuned by adjusting synthesis parameters. This synthesis method can also be extended for the fabrication of other mesoporous metal oxide materials.
2. Experimental Section
2.1. Synthesis of Mesoporous Nanocrystalline TiO2 Microspheres
All the reagents are analytical grate and were used without further purification (from Sinopharm Chemical Reagent Ltd.). In a typical procedure, 12 mmol urea was dissolved into 60 mL of absolute ethanol; then the solution was slowly added into the other solution (mixture of 20 mL ethanol, 2 mL tetrabutyl titanate (Ti(OC4H9)4), and 1 mL glacial acetic acid (CH3COOH)) under stirring. The solution was transferred into a 100 mL Teflon-lined autoclave after stirring for 30 min. The autoclave was put into an oven and maintained at 140°C for 20 h. The precipitate was rinsed by ethanol for several times, dried at 90°C for 12 h, and then calcined at 450°C for 2 h. For comparison, different amounts of urea were added while keeping other reaction conditions constant.
2.2. Characterization of Mesoporous Nanocrystalline TiO2 Microspheres
XRD measurements were performed on a Bruker D8 X-ray diffractometer with Cu-Kα radiation ( Å) at a scan rate of 4° min−1 at 45 kV and 40 mA.
The N2 adsorption-desorption isotherms of the TiO2 microspheres were obtained at −196°C using a Quantachrome Autosorb 1-C. Before measurements, samples were degassed under vacuum at 300°C for 4 hours. The Brunauer-Emmett-Teller (BET) approach was used to calculate specific surface area of the sample by using adsorption data over the relative pressure range of 0.05–0.30. The Barrett-Joyner-Halenda (BJH) approach was employed to determine pore size distribution and average mesopore diameter by using desorption data of the isotherms.
SEM images were obtained on a JEOL JEM 6360 scanning electron microscope with accelerating voltage of 20 kV.
3. Results and Discussion
3.1. Textural Properties
Figure 1 shows the XRD patterns of the TiO2 samples prepared with different amounts of urea. The strong and sharp peaks observed in Figure 1 confirm the catalysts are all well crystallized. For all samples, the diffraction peaks appear at 25.17°, 38.23°, 48.09°, 55.05°, 62.83°, 69.7° and 75.3°, all the peaks can be indexed to TiO2 phase (Anatase, JCPDS 21-1272), which corresponds to (101), (004), (200), (105), (204), (116), and (215) planes, respectively. No diffraction peaks of rutile TiO2 phase can be detected. The XRD results indicate the as-prepared TiO2 is of high purity. Normally, the rutile phase is more stable than the anatase phase. Here, the as-prepared TiO2 mesoporous microspheres are in anatase phase which could be ascribed not too high calcined temperature. The crystallite sizes of the synthesized TiO2 samples estimated from the Debye-Scherrer equation , using the XRD line broadening of (101) diffraction peak, are reported in Table 1. It can be seen from Table 1 that crystallite sizes slightly decreased from 12.2 nm to 8.7 nm, with increasing the amount of urea, indicating the decrease of crystallization of the TiO2 nanocrystals.
The morphology and size of the TiO2 samples were examined by SEM. Figures 2(a)–2(h) show that TiO2 microspheres with different sizes can be achieved accordingly by adjusting the amount of urea. When the amount of urea is 8 mmol, the size and surface structure of the microspheres can be observed in Figures 2(a) and 2(b). The TiO2 microspheres are found to be 1–6 μm in diameter, the surfaces of the microspheres are very smooth, and the mean size of the diameter is about 4 μm. It is clearly seen that the microspheres disperse well, but the sizes are not even. With the increasing amount of urea to 12 mmol (see Figures 2(c) and 2(d)), the mean diameter size of the TiO2 microspheres decreases to about 2-3 μm, and the sizes are relatively uniform. The morphologies and sizes of the TiO2 microspheres change little with increasing the urea amount to 16 mmol, as can be seen from Figures 2(e) and 2(f). However, if further increasing the urea amount to 20 mmol, it is observed from Figures 2(g) and 2(h) that “chain-like” and “peanut-like” TiO2 microspheres are obtained, replacing the dispersed microspheres; the diameter sizes of the microspheres decrease, ranging from 1 to 3 μm again. The result means that the amount of the urea can greatly affect the size of the products, and the size of the microspheres decreased with increasing the amount of urea. Interestingly, the microspheres structure can still maintain the morphology even after ultrasonication for 30 min, indicating the structure is stable.
3.3. Specific Surface Area and Pore Character of the TiO2 Microspheres
The microstructural characteristics of the TiO2 microspheres were further investigated with the N2 adsorption/desorption analysis. The adsorption isotherms of the TiO2 microspheres are shown in Figures 3(a)–3(d), respectively. All samples exhibit type IV adsorption isotherms with different types of hysteresis loop (lines in Figures 3(a) and 3(d with type H3, while lines in Figures 3(b) and 3(c) with type H2), typical for mesoporous materials . Usually, isotherms with type H3 hysteresis loop means the occurrence of irregular long and narrow pores, while with type H2 hysteresis loop mean the occurrence of regular “bottle-like” pores which exhibit a smaller size of opening but a larger size of inside chamber. With small amount of urea (8 mmol), the hysteresis loop ranges ; when , the adsorption increases significantly, indicating the existence of macropores with diameter of 10–100 nm . This speculation can also be proved from the corresponding wide pore size distribution as depicted in Figure 4(a). When the amount of urea increased to 12 mmol, the hysteresis loop also ranges ; at , the adsorption increases little, implying almost all mesoporous structure of the sample. The pore size distributes 3–20 nm, as depicted in Figure 4(b). If further increasing the amount of urea; for example, 16 mmol urea were used, and the hysteresis loop range of the sample also becomes narrow, only , which demonstrates the pore size distribution is relatively concentrated, as can be seen from Figure 4(c), ranging only 3-4 nm. However, with more amount of urea (20 mmol), although the hysteresis loop still exhibits a small triangular shape and a steep desorption branch like the sample prepared with 16 mmol, the pore size distribution becomes wide again. As indicated in Figure 4(d), there are two kinds of pore sizes, one is about 3–10 nm, and another is much larger than 30 nm (30–200 nm). It can be concluded that the amount of urea has a great influence on the pore size distribution of TiO2 microspheres. This result can be explained from the point view of the nucleation and growth process of the TiO2 microspheres. In our synthesis, urea can provide basic environment for the alcoholysis of Ti(OC4H9)4 to Ti(OH)4 and corresponding condensation. The overall growth mechanism of the TiO2 precursors could be divided into two stages: the initial formation of nuclei and the subsequent growth of nuclei. When the amount of urea is too small, the alcoholysis rate is considerably slower, which can incur the greater difference of the growth times for the particle; so the diameter size uniformity of the product is poor. In contrast, if the amount of urea is too large, the alcoholysis rate is fast enough so that all nuclei are formed at the initial stage, and nearly null particles are available for the subsequent nuclei growth. Accordingly, the nuclei aggregate to become spheres driven by minimization of surface energies according to the Gibbs-Thomson law; therefore the bigger microspheres grow up at the expense of disappearance of smaller ones, and the diameter size distribution is also poor. In addition, the amount of urea influences the condensation rate of Ti(OH)4, and the narrow pore size distribution can be obtained at suitable condensation rate. Our research results indicate nanocrystalline TiO2 mesoporous microspheres with controlled pore size distribution which can be synthesized by controlling the amount of urea.
It is also interesting to note that BET specific surface areas, pore volumes, and average pore diameters also changed with the amount of urea used in preparation, as shown in Table 1. The BET specific surface areas and pore volumes first increase and then decrease with the increasing amount of urea. The TiO2 samples prepared with 12 mmol urea exhibit the maximum BET surface area of 57.35 m2/g, which is a little larger than that of commercial P25 .
In summary, mesoporous TiO2 microspheres self-assembled from nanoparticles are synthesized by a surfactant-free Solvothermal method combined with postcalcination route. The as-prepared TiO2 microspheres show anatase phase, high degree of crystallinity, and large BET surface areas. By adjusting the amount of urea used in synthesis, the pore size distribution and the diameters of the mesoporous TiO2 microspheres can be tuned. The new approach could be extended to the fabrication of other metal mesoporous materials.
The authors thank Liaoning Science and Technology Department Foundation (no. 2007223016), Liaoning Educational Department Foundation (L2011065), Shenyang Science and Technology Department Foundation (no. F11-264-1-76), and Scientific Research Starting Foundation for Doctor, Liaoning Province (no. 20111046), for financial support.
- Y. J. Zhang, S. W. Or, and Z. D. Zhang, “Hydrothermal self-assembly of hierarchical cobalt hyperbranches by a sodium tartrate-assisted route,” RSC Advances, vol. 1, no. 7, pp. 1287–1293, 2011.
- J. Y. Cho, W. H. Nam, Y. S. Lim, W.-S. Seo, H.-H. Park, and J. Y. Lee, “Bulky mesoporous TiO2 structure,” RSC Advances, vol. 2, pp. 2449–2453, 2012.
- A. Wold, “Photocatalytic properties of TiO2,” Chemistry of Materials, vol. 5, no. 3, pp. 280–283, 1993.
- D. M. Antonelli and J. Y. Ying, “Synthesis of hexagonally packed mesoporous TiO2 by a modified sol-gel method,” Angewandte Chemie, vol. 34, no. 18, pp. 2014–2017, 1995.
- P. Kubiak, J. Geserick, N. Hüsing, and M. Wohlfahrt-Mehrens, “Electrochemical performance of mesoporous TiO2 anatase,” Journal of Power Sources, vol. 175, no. 1, pp. 510–516, 2008.
- D. Dambournet, I. Belharouak, and K. Amine, “Tailored preparation methods of TiO2 anatase, rutile, brookite: mechanism of formation and electrochemical properties,” Chemistry of Materials, vol. 22, no. 3, pp. 1173–1179, 2010.
- F. Liu, C.-L. Liu, B. Hu, W.-P. Kong, and C.-Z. Qi, “High-temperature hydrothermal synthesis of crystalline mesoporous TiO2 with superior photo catalytic activities,” Applied Surface Science, vol. 258, no. 19, pp. 7448–7454, 2012.
- K. H. Lee and S. W. Song, “One-step hydrothermal synthesis of mesoporous anatase TiO2 microsphere and interfacial control for enhanced lithium storage performance,” ACS Applied Materials & Interfaces, vol. 3, no. 9, pp. 3697–3703, 2011.
- Z. Bian, J. Zhu, F. Cao, Y. Huo, Y. Lu, and H. Li, “Solvothermal synthesis of well-defined TiO2 mesoporous nanotubes with enhanced photocatalytic activity,” Chemical Communications, vol. 46, no. 44, pp. 8451–8453, 2010.
- Y. Zhang, L. Wu, Q. Zeng, and J. Zhi, “An approach for controllable synthesis of different-phase titanium dioxide nanocomposites with peroxotitanium complex as precursor,” Journal of Physical Chemistry C, vol. 112, no. 42, pp. 16457–16462, 2008.
- M. G. Choi, Y. G. Lee, S. W. Song, and K. M. Kim, “Lithium-ion battery anode properties of TiO2 nanotubes prepared by the hydrothermal synthesis of mixed (anatase and rutile) particles,” Electrochimica Acta, vol. 55, no. 20, pp. 5975–5983, 2010.
- A. R. Armstrong, G. Armstrong, J. Canales, and P. G. Bruce, “TiO2-B nanowires,” Angewandte Chemie, vol. 43, no. 17, pp. 2286–2288, 2004.
- M. Alvaro, C. Aprile, M. Benitez, E. Carbonell, and H. García, “Photocatalytic activity of structured mesoporous TiO2 materials,” Journal of Physical Chemistry B, vol. 110, no. 13, pp. 6661–6665, 2006.
- H. Shibata, T. Ogura, T. Mukai, T. Ohkubo, and H. Sakai, “Direct synthesis of mesoporous titania particles having a crystalline wall,” Journal of the American Chemical Society, vol. 127, no. 47, pp. 16396–16397, 2005.
- S. Li, Q. Shen, J. Zong, and H. Yang, “Synthesis of size-tunable mesoporous anatase titania spheres by a template-free method,” Materials Research Bulletin, vol. 45, no. 7, pp. 882–887, 2010.
- K. Yoo, H. Choi, and D. D. Dionysiou, “Ionic liquid assisted preparation of nanostructured TiO2 particles,” Chemical Communications, vol. 10, no. 17, pp. 2000–2001, 2004.
- J. Wang, Y. Zhou, Y. Hu, R. O'hayre, and Z. Shao, “Facile synthesis of nanocrystalline TiO2 mesoporous microspheres for lithium-ion batteries,” Journal of Physical Chemistry C, vol. 115, no. 5, pp. 2529–2536, 2011.
- S. K. Das, M. Patel, and A. J. Bhattacharyya, “Effect of nanostructuring and ex situ amorphous carbon coverage on the lithium storage and insertion kinetics in anatase titania,” ACS Applied Materials and Interfaces, vol. 2, no. 7, pp. 2091–2099, 2010.
- Y. J. Kim, S. Y. Chai, and W. I. Lee, “Control of TiO2 structures from robust hollow microspheres to highly dispersible nanoparticles in a tetrabutylammonium hydroxide solution,” Langmuir, vol. 23, no. 19, pp. 9567–9571, 2007.
- S. Lowell, J. E. Shields, and M. A. Thomas, Characterization of Porous Solids and Powders: Surface Area, Pore Size and Density, Kluwer Academic Publishers, Dordrecht, The Netherlands, 2004.
- G. Calleja, D. P. Serrano, R. Sanz, P. Pizarro, and A. García, “Study on the synthesis of high-surface-area mesoporous TiO2 in the presence of nonionic surfactants,” Industrial and Engineering Chemistry Research, vol. 43, no. 10, pp. 2485–2492, 2004.
- S. Sakulkhaemaruethai and T. Sreethawong, “Synthesis of mesoporous-assembled TiO2 nanocrystals by a modified urea-aided sol-gel process and their outstanding photocatalytic H2 production activity,” International Journal of Hydrogen Energy, vol. 36, no. 11, pp. 6553–6559, 2011.