Lei Zenga,
Wulin Song*ab and
Changsheng Xiea
aState Key Laboratory of Materials Processing and Die & Mould Technology, Huazhong University of Science and Technology, P. R. China. E-mail: wulins@126.com; Tel: +86-27-87557453
bAnalytical and Testing Center, Huazhong University of Science and Technology, P. R. China
First published on 30th July 2014
Here, we report a special rod in tube nanostructured TiO2 prepared by a moderate esterification reaction. The morphology evolution with reaction time was observed by FSEM and FETEM. Comparing to the as-reported sphere in sphere nanostructured TiO2, the formation of a rod in tube nanostructure was attributed to the use of a solid precursor. The nucleation-dissolution-anisotropic grain growth-recrystallization mechanism is responsible for the formation of the rod in tube nanostructure. Moreover, the photocatalytic properties of different morphologies of samples were also compared, indicating that the rod in tube nanostructured TiO2 possessed the best photocatalytic activity. The improvement of photocatalytic activity is mainly attributed to the enhancement of light-harvesting and the separation of electron–hole pairs. Finally, the present work also provided a template-free method to synthesize hierarchical porous TiO2 nanotube through prolonging reaction duration.
For the synthesis of TiO2 nanomaterial, researchers have developed many effective methods, such as hydrothermal, sol–gel, chemical vapour deposition and magnetron sputtering et al. The chemical synthesis method is the most economical and extensively used tool. However, most of chemical synthesis protocols need to use precursor. The widely used precursor contains titanium alkoxide and inorganic substance with titanium. So far, lots of publications have reported that the use of different kinds of precursor induce the formation of TiO2 with various morphology, size and crystal phase. For example, the porous, sheet, tubular and complex hierarchical structure (anthoid, yolk, dendritic et al.) TiO2 have been prepared by adjusting pH value, solvent composition, reaction duration and temperature.6–10 In addition, demand for high efficient photocatalyst determines the development of many convenient and valid preparation methods. These methods must effectively enhance specific surface area and improve the separation of electron–hole pairs. Obviously, the one-dimensional tubular structure achieves the requirements. Nonetheless, most of the synthesis of tubes needs to use templates or toxic chemicals, even for a tedious process.11–19 Hence, it is necessary to search an eco-friendly, template-free and simple protocol to prepare TiO2 nanotube.
In the present work, a mesoporous titania nanotube with tunable chamber structure has been generated by using a template-free method which is inspired by Li.20 To our surprise, the sphere in sphere structure is not generated whereas the rod in tube structure forms since the precursor is TiOSO4 powders. Hence, the effect of different states of precursor on the morphology of TiO2 and the relative formation mechanism is also investigated. In addition, the comparison of the as-prepared samples with different morphologies shows that the special rod in tube structure TiO2 possesses the best photocatalytic activity towards degradation of gaseous benzene, and the relative reason is also explained.
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Fig. 1 The electron micrographs of titania rods synthesized for 2 h (A and D), 48 h (B and E), 192 h (C and F). |
Fig. 2 displays the XRD pattern for the above three samples. It is clear to see that all samples show the similar pattern which can be indexed to anatase (JCPDS file no. 21-1272) and rutile (JCPDS file no. 21-1276), which is consistent with TEM. The trace of rutile can be attributed to the calcination at 550 °C.21 It is favourable to form rutile at high temperature (>500 °C).
Interestingly, when liquid tetrabutyl titanate was chose to be precursor and reacted at the absolutely identical condition, the clubbed structure was not obtained whereas the spherical structure appeared. After 48 h reaction (denoted as ST-48), the sphere in sphere structure formed (Fig. 3). An urchin like prickly sphere was also observed, and the diameter was around 600 nm as well as the thickness of shell was about 80 nm. From the inset of Fig. 3, it is apparently to know that the ST-48 was also mainly comprised of anatase. The XRD pattern of ST-48 was demonstrated in Fig. S2,† indicating that the ST-48 was also consisted of anatase and rutile. The maximum proportion of rutile phase was 8.7 wt% calculated by the widely used equation X = 1/(1 + 0.8IA/IR), where IA and IR were the diffraction intensities corresponding to the anatase (101) plane and the rutile (110) plane respectively.22 For the T-48 samples, the maximum proportion of rutile phase was 8.1%. The difference of phase composition between ST-48 and T-48 sample was not significant.
N2 sorption isotherms display type-IV curves which the capillary condensation phenomenon appears at relative high pressure for T-2, T-48 and ST-48 sample, characteristic of mesoporous solids with uniform pore sizes (Fig. 4).23–25 This is coincident with TEM results. The pore-sizes distribution curves with a mean value of about 15 nm are calculated from the adsorption branches based on the BJH mode for T-2 sample. After 48 h reaction, the average value of pore size is still around 15 nm whereas the pore-size distribution has narrowed. It might be because the grains grow up and the pore formed by grains stacking becomes smaller. For T-192 sample, the BET surface area cannot measure by using single-point BET method. It may be ascribed to the hollow tubular structure exist in T-192, which is verified by TEM observation. The macropore need be measured by using mercury intrusion method. For ST-48, the pore-sizes distribution is wide. However, the BET surface area of T-2, T-48 and ST-48 is 67.3 cm2 g−1, 65.9 cm2 g−1 and 25.8 cm2 g−1, respectively.
The PL spectrum is an effective way to investigate the electronic structure, optical and photochemical properties of semiconductor materials as well as the efficiency of charge carriers trapping, immigration and transfer can be also obtained. In our experiment, the PL spectrum of four samples is shown in Fig. 5. All samples can exhibit a strong and wide PL signal at the range from 380 to 750 nm, with the excitation light of energy higher than the bandgap energy, having two obvious PL peaks at about 425 and 575 nm, respectively, which are attributed to excitionic PL. The stronger the PL signal, the higher the combination rate of photo-induced charges is.
The result from Li's experiment show that the formation of titania spheres with sphere in sphere structure is not affected by the kinds of precursor. Comparing to that, the present work imply that the morphology is dependent on state of precursor. When liquid precursor is used in this experiment, the titania spheres with sphere in sphere structure tend to form. If solid precursor is used in the reaction, it is conductive to obtain the titania tubes with rod in tube structure. The formation mechanism is illustrated in Fig. 6. During the solventhermal reaction, the water was produced continuously by etherifying reaction between alcohol and glycerol. TiO2 building clusters was generated by hydrolysis–condensation reactions of precursor (titanium alkoxide or titanium inorganic salt). Then the as-formed clusters aggregated and self-assembled. When liquid precursor is used, the generated TiO2 crystal nucleus is tiny. Moreover, the tiny crystal tends to aggregate to cluster in order to minimum the surface energy. More importantly, the anisotropic grain growth is inhabited. Hence, the spherical structure is formed. For the solid precursor, it can be explained by nucleation-dissolution-anisotropic grain growth-recrystallization mechanism. The solid precursor powders suspend in the solvent as seed crystals. It is not restricted to anisotropic grain growth for the large scale crystal. As the reaction progress, the grains stack each other and self-assemble to form a rod. Meanwhile, water is generated continuously and reacts with the spheres and rods, leading to the dissolution and rearrangement of the surface building clusters. As a result, the core–shell structure appears. Continuation of this process, the core dissolves gradually. The hollow structure creates at last.
The photocatalytic activity toward decomposing benzene under UV-light is demonstrated in Fig. 7. Apparently, the blank experiment shows benzene cannot be decomposed without using photocatalyst under UV light illumination. It is evident that the sample T-48 is the most active photocatalyst among these samples. The concentration of benzene has reduced to 32.3%, 28.6%, 82.7% and 44.3% for T-2, T-48, T-192 and ST-48, respectively. In addition, the trend of photocatalytic activity is not absolutely identical to that of specific surface area and is not consistent with the result from Li's experiment, either. The specific surface area of T-2 is larger than T-48 while the photocatalytic activity of T-2 is worse. Importantly, the outside surface area can be obtained by BET measurement. The surface of T-2 is comprised of nanoparticle. The porous formed by the stacking of nanoparticles have a great contribution to the surface area. More importantly, the enhancement of photocatalytic activity of T-48 is ascribed to the multiple reflections of UV light within the tube interior voids, viz. the improvement of light-harvesting of T-48 (ref. 26–28) and the high separation rate of photo-induced charges. Thus, T-48 samples possess the best photocatalytic activity among all samples.
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Fig. 7 Catalytic oxidation of benzene (left) and CO2 generation (right) using four samples under UV light illumination. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra06086e |
This journal is © The Royal Society of Chemistry 2014 |