Hailong Penga,
Xiaoyan Yangb,
Peng Zhangc,
Yiming Zhanga,
Chengwei Liua,
Dan Liu*a and
Jianzhou Gui*ac
aState Key Laboratory of Separation Membranes and Membrane Processes, College of Environment and Chemical Engineering, Tianjin Polytechnic University, Tianjin 300387, China. E-mail: jzgui@hotmail.com; ldan2000@163.com; Tel: +86-022-83955668
bSchool of Chemistry and Chemical Engineering, Shangqiu Normal University, Shangqiu 476000, China
cSchool of Material Science and Engineering, Tianjin Polytechnic University, Tianjin 300387, China
First published on 27th October 2017
A simple diethylenetriamine (DETA)-assisted solvothermal method is utilized for in situ synthesis of TiO2 nanoparticles on carbon nanotubes (CNTs), fabricating TiO2/CNT composites with well-defined structure and enhanced photocatalytic activity for the degradation of methylene blue (MB). It is found that the DETA plays an important role on the structure, photoelectrochemistry and catalytic performance of the TiO2/CNT composites. Particularly, the TiO2/CNT catalyst obtained in the presence of 0.02 mL DETA exhibits both a low adsorption capacity and high photodegrading activity for MB removal under the UV-light irradiation, proving the uniform and well-dispersed TiO2 particles loaded. Systematic characterization reveals the strong interaction and high electron-transfer efficiency between TiO2 and CNT in the sample with the assistance of DETA. Besides, a DETA-assisted formation mechanism of the TiO2/CNT composite has also been proposed in this study: DETA will work as a connecting bridge to facilitate the uniform adsorption of Ti4+ on the surface of CNT. With the increase of solvothermal temperature, the adsorbed Ti4+ gradually in situ crystallizes to form the TiO2/CNT composite. The DETA-assisted in situ synthesis could be expected to be a promising method for the preparation of metal oxides supported on carbon materials with well-defined structure and superior photocatalytic or photoelectrochemical properties.
It is found that the hybridization of carbon materials can greatly enhance the photocatalytic activity of TiO2.16–20 On the one hand, as catalyst supports, the carbon materials can disperse and anchor TiO2 particles to exhibit more catalytic active sites. On the other hand, benefiting from the high electrical conductivity, the carbon materials can effectively capture the photogenerated electrons on the surface of TiO2, prolonging the lifetime of oxidative active species.21 Among the selectable carbon materials, carbon nanotube (CNT) is regarded as a promising carbon material to be combined with TiO2, due to the large surface area, strong adsorption effect, and high structural flexibility.22,23 Baiju K. Vijayan et al.24 utilized a simple hydration/dehydration method to prepare CNT/TiO2 composites, which show great photocatalytic activity for degradation of acetaldehyde. Taicheng An et al.25 reported that TiO2 spheres with controllable crystallite size and dominant crystal facets such as {001}, {101}, or polycrystalline were successful supported on CNT, exhibiting the significant synergistic effect and enhanced photocatalytic efficiency. Jing Di et al.26 successfully synthesized plant leaf-shape TiO2 supported on CNT, which features not only a large specific surface area, but also a high light absorption due to the great scattering ability. Although some efforts have been devoted in previous works, due to the hydrophobicity, CNT shows a poor dispersity in water27 and a bad combination with metal cations, making it very difficult to uniformly deposit metal oxide on the surface. Up to now, it is still a big challenge to fabricate the TiO2/CNT composite photocatalyst with the uniformly loaded and structural controllable TiO2 particles, as well as the high photocatalytic performance.
Herein, a simple and facile solvothermal method is utilized to prepare TiO2 nanoparticles supported on CNT with the assistance of DETA. By tuning different precursor (isopropyl titanate, CNT, DETA), a group of TiO2/CNT composites have been separately obtained, and their adsorption capacity and photodegrading activity for MB removal were evaluated in detail. It is found that DETA greatly affect the loading uniformity and dispersity of TiO2 particles supported, and the TiO2/CNT composite with 0.02 mL DETA added shows a strong interaction and the rapid electron-transfer efficiency between TiO2 and CNT. Moreover, a possible DETA-assisted formation mechanism of the TiO2/CNT composite has also been proposed in this work.
Three colorless antibiotics were also used as a target for photodegradation. In the reaction, 0.01 g sample was dispersed in three antibiotics solution (20 mg L−1 tetracycline (TC), 20 mg L−1 enrofloxacin hydrochloride (ENRH) and 10 mg L−1 ciprofloxacin (CIP)) and magnetically stirred for 30 min in dark to achieve the adsorption/desorption equilibrium. And then, the photocatalytic experiment began at the same condition. About 4 mL mixture was taken out per 20 minutes, and then centrifugal separation to obtain the reaction solution. The catalytic activity of different samples was evaluated by C/C0, where C0 was the three colorless antibiotics (TC, ENRH and CIP) absorbance of initial solution at 357, 273 and 273 nm, and C was the three colorless antibiotics real-time absorbance of reaction solution.
Scheme 1 Adsorption and photocatalytic processes of TiO2/CNT composite for the MB removal under UV-light irradiation. |
A series of TiO2/CNT composites have been prepared by tuning three precursor amounts, i.e. isopropyl titanate (IT), CNT, and DETA. Their theoretical chemical compositions have been summarized in Table S1,† and the adsorption capacity and photocatalytic activity have also been investigated systematically, as shown in Fig. 1.
By changing the weight ratio of TiO2 from 71% to 91% (Table S1†), the 0.04-TixC67 composites generally exhibit the similar MB-removed efficiency, as shown in Fig. 1a. By the plots of ln(C/C0) vs. illumination time (Fig. 1d), the first-order linear relationship could be found in all the four samples, of which the undistinguishable fitting-line slopes imply the similar photocatalytic activity of the 0.04-TixC67 composites. From the relationship between the adsorption and catalytic capability (Fig. 1g), it can be clearly seen that the 0.04-Ti1.2C67 shows slightly enhanced catalytic performance compared with others, as well as the remarkably lower adsorption capacity. Obviously, the TiO2 overloaded in TiO2/CNT composite may greatly affect the loading uniformity of TiO2 particles due to their aggregation, whereas exhibiting a negligible difference for their photocatalytic activity.
By increasing CNT amount, the adsorption capacity of corresponding samples firstly decreased and then increased, while their catalytic activity has the reverse trend (Fig. 1b, e and h). As shown in Fig. 1h, when the additive amount of CNT is 67 mg, the 0.04-Ti1.2C67 has the lowest adsorption for MB, indicating the highest coverage proportion among these samples. As the CNT content continuously increasing, more TiO2 active sites will be exposed, resulting in the increasing photocatalytic activity. Therefore, although improving the dispersity of TiO2 nanoparticles, the increase of CNT content seems not to improve their uniformity simultaneously, which fails to fabricate the TiO2/CNT composite with well-defined structure.
In addition, DETA in the system also plays an important role in controlling the structure of TiO2/CNT composite. As shown in Fig. 1c, the MB-removed efficiency of the 0.01-Ti1.2C67 and 0.02-Ti1.2C67 is much higher than that of the 0-Ti1.2C67, mainly owning to their greatly enhanced photocatalytic performance (Fig. 1f). Fig. 1i shows that the two TiO2/CNT composites have a gradually decreasing adsorption for MB with the DETA amount, indicating that the introduce of DETA can effectively promote the TiO2 loading uniformity. However, excess DETA, in the case of 0.04-Ti1.2C67, inversely leads to the obvious decrease in photocatalytic performance, meanwhile it exhibits the lowest adsorption capacity compared with other samples. Therefore, the appropriate DETA will play an important role in fabricating the TiO2/CNT composite with both the great TiO2 loading uniformity and the high dispersity.
Besides MB, the 0.02-Ti1.2C67 also exhibits a great photocatalytic performance for the degradation of colorless organics (TC, ENRH, CIP), the reaction processes of three antibiotics have shown in Fig. 2. Obviously, three antibiotics are found to be rapidly degradated over the 0.02-Ti1.2C67 under the UV irradiation, which removes almost 99% TC, 94% ENRH and 95% CIP after exposed in UV light for 120 min. It is indicated that the resultant 0.02-Ti1.2C67 has a good photocatalytic efficiency for many organic molecules.
Fig. 2 Photocatalytic degradation of three antibiotics (TC, ENRH, CIP) over 0.02-Ti1.2C67 under UV-light irradiation. |
From Fig. 3b, we can clearly see that the 0-Ti1.2C67 and 0.02-Ti1.2C67 show the coincident N2 adsorption–desorption isotherms, and their BET surface areas have been estimated to be 138.863 m3 g−1 and 147.217 m3 g−1, respectively.
SEM images of the two samples loaded by TiO2 particles with/without the assistance of DETA (0.02-Ti1.2C67 and 0-Ti1.2C67) have been shown in Fig. 4a and b, both the two samples have partially maintained the initial wire-type morphology of CNT (Fig. S4†), illustrating that CNT works as the framework in the fabrication of the TiO2/CNT composite. Particularly, the 0.02-Ti1.2C67 displays a highly entangled one-dimensional parasitic architecture with a 40–45 nm diameter size, which is slightly larger than the pure CNT (30–35 nm). On the contrary, a cluster of TiO2 particles could be clearly observed in the 0-Ti1.2C67 (Fig. 4b), through a lot of coarse nanowires are also presented in the appearance. The detailed structure of the two products would be revealed by the corresponding TEM images (Fig. 4c and d). For the sample 0.02-Ti1.2C67, TiO2 particles are evenly grown along the CNT, whereas the 0-Ti1.2C67 has both the badly aggregated TiO2 particles and the bare CNT. From the SEM and TEM images, it is indicated that the TiO2 loading uniformity of the TiO2/CNT composite could be significantly improved, when DETA is introduced into the solvothermal system. This structural difference can also be seen from their HRTEM images (Fig. 4e and f). As shown, compared with the 0-Ti1.2C67, the 0.02-Ti1.2C67 possesses the well-dispersed TiO2 particles on the CNT. Moreover, the clear lattice fringes with interplanar spacing of 0.354 nm and 0.356 nm are found in two HRTEM images, which match well with the TiO2 (101) lattice plane. Obviously, in spite of the different uniformity and dispersity, TiO2 particles in two samples (Fig. 4e and f) show a high crystallinity and the same crystal structure.
XPS is conducted to further distinguish the structural difference between the 0.02-Ti1.2C67 and 0-Ti1.2C67, and the detailed results have been displayed in Fig. 5. From their XPS survey spectra (Fig. 5a), we can see the identical peaks in both XPS spectra, indicating the similar general structure. Besides, the 0.02-Ti1.2C67 and 0-Ti1.2C67 also exhibit the same high-resolution XPS spectra of Ti (Fig. 5b), in which two bands centered at 458.6 and 464.3 eV correspond to Ti(IV) 2p1/2 and Ti(IV) 2p3/2,29–31 respectively. However, as shown in Fig. 5c, the peak at 532.1 eV assigned to C–O–Ti could be clearly observed in XPS spectrum of O 1s of the 0.02-Ti1.2C67, which is much stronger than that of 0-Ti1.2C67. This result demonstrates that an interaction excits between CNT and TiO2 in the 0.02-Ti1.2C67. Meanwhile, due to the extensive coverage of TiO2 particles, there are a lot of oxygen-containing groups reserved on CNT, thus a peak from C–O or CO (533.5 eV) is also presented in the 0.02-Ti1.2C67.31–33 Consistence with the XPS result of O 1s, the 0.02-Ti1.2C67 also has an additive peak at 288.9 eV in the XPS spectrum of C 1s (Fig. 5d), which can be attributed to the Ti–O–C,34–37 further indicating the strong interaction between TiO2 and CNT in the 0.02-Ti1.2C67. Moreover, the detailed chemical compositions of the 0.02-Ti1.2C67 and 0-Ti1.2C67 analyzed by XPS have been summarized in Tables S2 and S3,† respectively.
Fig. 5 (a) XPS survey spectra of 0.02-Ti1.2C67 and 0-Ti1.2C67; high-resolution XPS spectra of (b) C 1s; (c) O 1s; (d) Ti 2p of 0.02-Ti1.2C67 and 0-Ti1.2C67. |
In UV-DRS of the 0-Ti1.2C67 and 0.02-Ti1.2C67 (Fig. 6a), both a strong absorption in UV region (below 400 nm) and visible absorption in 400–800 nm could be observed, while the 0.02-Ti1.2C67 shows a stronger visible absorption compared with the 0-Ti1.2C67, probably because of its high dispersity of TiO2 particles on CNT. However, from the plots of (αhν)2 versus (hν),38 we can find no obvious difference between the band gap energy (Eg) of 0-Ti1.2C67 and 0.02-Ti1.2C67, indicating no effect of DETA on the band gap of TiO2/CNT composites.
PL is a powerful tool to analyze the essential optical property of photocatalysts. Fig. 7 compares PL spectra of the 0-Ti1.2C67 and 0.02-Ti1.2C67 at an excitation wavelength of 294 nm, both of which include an emission peak at ca. 396 nm and series of peaks in the range of 440–500 nm. Generally, the strong peak at ca. 396 nm is attributed to the electron transition of the bandgap energy of anatase TiO2 (∼397 nm),39,40 while peaks ranging from 440 to 500 nm are ascribed to the electron migration resulted from the surface defects.41 For the 0.02-Ti1.2C67, the quenching fluorescence indicates a faster transfer of surface electrons than the 0-Ti1.2C67, resulting from the close contact between TiO2 and CNT. Therefore, the 0.02-Ti1.2C67 has exhibited the superior photocatalytic activity in the photodegradation of MB under the irradiation of UV-light. Meanwhile, the equivalent emission peaks from 440–500 nm can be clearly seen in two samples, indicating the similar TiO2 surface structure, which is very agreement with the XPS result discussed above. PL analysis of all samples obtained in this work (Fig. S5†), it is found the CNT and DETA play an important role on the electron transport efficiency of the TiO2/CNT composites, which well matches with the photocatalytic experimental results. However, the decreasing PL emission peak probably attribute to the increasing amount of CNT in samples. As for z-Ti1.2C67 samples, a declining PL peak has been observed in the 0.02-Ti1.2C67, indicating that when the additive amount of DETA is 0.02 mL, the corresponding product possesses the higher electron-transfer rate from TiO2 particles to CNT.
Furthermore, the photoelectrochemical property of two TiO2/CNT composites are investigated by their photocurrent responses and EIS, and the detailed results have been displayed in Fig. 8. From Fig. 8a, we can clearly see that both the 0-Ti1.2C67 and 0.02-Ti1.2C67 have transient photocurrent responses in three on–off cycles of UV-light irradiation in 0.1 M Na2SO4 solution, resulting from the separation of photogenerated electron/hole pairs in two samples. In comparison to the 0-Ti1.2C67, the photocurrent density of the 0.02-Ti1.2C67 is much higher, demonstrating an increasing electron-transfer efficiency. Consequently, in the 0.02-Ti1.2C67, the close contact between TiO2 and CNT successfully facilitates the migration efficiency of surface electrons. Meanwhile, both the 0.02-TixC67 and 0.02-Ti1.2Cy samples have the similar photocurrent intensity, as shown in Fig. S6.† It is demonstrated that the electron-migration efficiency of TiO2/CNT composites cannot be greatly affected by the amounts of CNT and TiO2 particles in system. On the contrary, DETA is the major influence factor to the materials which can be seen from the great difference photocurrent response.
Fig. 8 Photocurrent responses (a) and Nyquist plots (b) of 0-Ti1.2C67 and 0.02-Ti1.2C67 in 0.1 M Na2SO4 solution under UV-light irradiation. |
To further analyze the surface charge migration, EIS of the 0-Ti1.2C67 and 0.02-Ti1.2C67 were measured in 0.1 M Na2SO4 solution, both in dark and under the irradiation of UV-light. For photocatalysts, the Nyquist plot recorded in dark can represent their intrinsic charge-transfer resistance. From Fig. 8b, the identical Nyquist plot in dark indicates that the 0-Ti1.2C67 and 0.02-Ti1.2C67 have the similar CNT and TiO2 contents. After exposed to UV-light, the charge migration rate of the two samples have been dramatically accelerated, thus showing two depressed semicircles in the corresponding Nyquist plots. Particularly, the 0.02-Ti1.2C67 has the smaller radius than the 0-Ti1.2C67, verifying a higher charge migration efficiency. Consequently, the photoelectrochemical result agrees fairly well with the photocatalytic performance of the 0-Ti1.2C67 and 0.02-Ti1.2C67.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra09324a |
This journal is © The Royal Society of Chemistry 2017 |