Zemin
Dong
*ab,
Rendan
Zhou
c,
Leyan
Xiong
*a,
Han
Li
d,
Qiang
Liu
a,
Longzhen
Zheng
a,
Zanru
Guo
a and
Zhaoxiang
Deng
e
aDepartment of Chemistry and Chemical Engineering, East China Jiao Tong University, Nanchang 330013, P. R. China. E-mail: xly12@ecjtu.edu.cn; zemin1987d@139.com
bJiangXi Institute for Veterinary Drug and Feedstuffs Control, Nanchang 330096, PR China
cAnalysis and Testing Center, Nan Chang University, Nanchang 330047, P. R. China
dCAS Key Laboratory of Crust-Mantle Materials and Environments, School of Earth and Space Sciences, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China
eDepartment of Chemistry, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China
First published on 12th December 2019
A Ti0.7W0.3O2/TiO2 nanocomposite interfacial photocatalyst was designed and prepared for the photocatalytic degradation of phenol pollutants in wastewater. The detailed properties of the Ti0.7W0.3O2/TiO2 nanocomposite interface (NCI) were analyzed by XRD, SEM, EDX, DRS, UPS and XPS technologies, showing that anatase TiO2 nanospheres (NSs) were uniformly dispersed on the surface of rutile Ti0.7W0.3O2 nanoparticles (NPs) and formed the nanocomposite interface. The DRS and UPS results of 5 wt% Ti0.7W0.3O2/TiO2 NCI indicated a greatly broadened light response range with a wavelength shorter than 527 nm and a shorter band gap energy of 2.37 eV. The conduction band of TiO2 NSs, Ti0.7W0.3O2 NPs and 5 wt% Ti0.7W0.3O2/TiO2 NCI were measured based on the results of the valence band and band gap energy obtained via XPS and DRS, and then the energy level diagram of Ti0.7W0.3O2/TiO2 NCI was proposed. The photocatalytic degradation of phenol at Ti0.7W0.3O2/TiO2 NCI with different loading ratios of Ti0.7W0.3O2 NPs was investigated under optimum conditions (i.e., pH of 4.5, catalyst dosage of 0.45 g L−1 and phenol initial concentration of 95 ppm) under the illumination of ultraviolet visible light. Also, 5 wt% Ti0.7W0.3O2/TiO2 NCI exhibited the highest photocatalytic activity, with the initial rate constant (k) calculated as 0.09111 min−1. After recycling six times, Ti0.7W0.3O2/TiO2 NCI showed good stability and recyclability. The involvement of superoxide radicals in the initial reaction at Ti0.7W0.3O2/TiO2 NCI was evidenced by the use of a terephthalic acid (TA) fluorescent probe. Besides, UV-Vis spectroscopy, UHPLC-MS and GC-MS technologies were used to analyze the main intermediates in the photocatalytic degradation of phenol. The probable photocatalytic degradation mechanism of phenol at Ti0.7W0.3O2/TiO2 NCI was also proposed.
Among oxide semiconductor photocatalysts, TiO2 nanomaterials have been studied and applied widely in photocatalysis for their high photocatalytic activity, stability, nontoxicity and low cost. A variety of functional TiO2 nanomaterials have been synthetized, such as nanoparticles (NPs),4–9 nanotubes (NTs),10,11 nanowires (NWs),12–15 nanocrystal films16–20 and nanotube arrays,21–25 which have been widely used in solar energy storage and utilization, photodegradation of pollutants and noble metal recycling.
However, the total quantum efficiency of TiO2 is very low,26–28 which has limited the potential value of actual production and application of TiO2 nanomaterials. A lot of studies have been done to address the drawbacks mentioned above, with noble metal deposition considered as one of the most effective and promising solutions. Pt is one such representative noble metal, which has been widely used to improve the performance of TiO2 nanomaterials in wastewater treatment and air purification with a superior performance. Wang29 successfully synthesised a Pt/TiO2 NW photocatalyst. The recombination rate of electrons and holes was reduced greatly for Pt NPs, resulting in good conductivity. Pt NPs are superior electron acceptors on the photocatalyst surface and enable the timely transfer of electrons. Emilio et al.30 observed an increase in the lifetime of electrons by Pt modification on the TiO2 surface due to the better separation of charge carriers caused by the Schottky barrier between Pt and TiO2. As expected, this helped to enhance the photocatalytic efficiency of TiO2.5–9,11,14,15,19,20,22,25,31–33 However, noble metals are scarce and particularly expensive, which may limit their large-scale application. Thus, novel relatively economical photocatalysts are highly desirable.
In the present paper, a Ti0.7W0.3O2/TiO2 NCI was synthesized via a sol–gel and combustion technique, and was shown to possess several positive aspects, such as good stability, good visible light response range and effectively decreased recombination of charge carriers by a fast photogenerated electron transfer. The photocatalytic activity of the Ti0.7W0.3O2/TiO2 NCI was investigated for the degradation of phenol under simulated solar light illumination, and it showed higher photocatalytic activity. Furthermore, the main intermediates and mechanism for the photocatalytic degradation of phenol at the Ti0.7W0.3O2/TiO2 NCI were also analyzed and discussed. This type of a photocatalyst may find application in low concentration organic wastewater clean-up.
Meanwhile, the detailed information on the characterization, photocatalytic test and analysis of the intermediates in the photocatalytic degradation of phenol are shown in ESI (Section 2†).
D = Kλ/βcosθ | (1) |
The average particle size and distribution of the anatase TiO2 NSs and Ti0.7W0.3O2 NPs were obtained using a laser particle size analyzer and are shown in ESI (Section 3, Fig. S6†). The average particle size and distribution of anatase TiO2 NSs were determined to be about 287 nm, which was larger than the average crystalline size calculated from the major diffraction peak (101) in the XRD analysis. The average particle size and distribution of Ti0.7W0.3O2 NPs were determined to be about 1189 nm, which was consistent with the result calculated from the major diffraction peak (110) in the XRD analysis of the rutile Ti0.7W0.3O2 NPs. The possible reasons for the deviation were as follows. On the one hand, some TiO2 NSs reunite after high temperature calcination. On the other hand, the principles of the two kinds of detection methods were different, whereby the results of the XRD analysis were estimated using an empirical formula, whereas the laser particle size analyzer detection needed the samples to be dispersed in water, and the dispersion of the TiO2 NSs was not very good and they were prone to reunion. This might lead to an increase in the error of the result.
Obviously, some diffraction peaks of Ti0.7W0.3O2 NPs (h) were slightly shifted due to doping with W4+ compared with pure rutile TiO2 (i). This phenomenon indicated an expansion of the a-axis and a contraction of the c-axis due to W–W pairing in the doped compound, which has also been observed in WO2/TiO2 nanocomposites.40–45 Meanwhile, the diffraction peaks for O2−–W4+ were very weak, demonstrating the low levels of W4+.
The PXRD patterns of Ti0.7W0.3O2/TiO2 NCI loaded with 1 wt%, 2 wt%, 5 wt%, 10 wt%, 20 wt% and 50 wt% Ti0.7W0.3O2 NPs are shown in Fig. 1(A)(b–g). All the samples were identical with the pure anatase and rutile phase after calcination at 400 °C, respectively. None of the diffraction peaks were changed significantly after deposition, which indicated that the Ti0.7W0.3O2 NPs did not affect the phase structure and chemical composition of the TiO2 NSs. However, further observation showed that the diffraction peaks corresponding to TiO2 NSs exhibited relatively weaker peak intensities and broader diffraction peak widths. It could be inferred from this that the average crystallite size was slightly decreased by Ti0.7W0.3O2 NPs modification, indicating that the Ti0.7W0.3O2 NPs have a negative effect on the grain growth of TiO2 NSs. This is because the Ti0.7W0.3O2 NPs restrained the crystal growth in the solids by providing dissimilar boundaries and hindered the mass transportation, thus resulting in smaller crystallite sizes.46 Meanwhile, no diffraction peaks of Ti0.7W0.3O2 NPs were observed up to 10 wt% (e), indicating that the TiO2 NSs were uniformly dispersed on the surface of the Ti0.7W0.3O2 NPs.
The superimposed PXRD patterns for the Ti0.7W0.3O2/TiO2 NCI before and after six cycles of irradiation are shown in Fig. 1(B). It is obvious that the two PXRD patterns almost overlap, which indicates that the stability of the Ti0.7W0.3O2/TiO2 NCI was encouraging, with less decomposition, thus accounting for the higher photocatalytic activity. A feeble and relatively weaker peak intensity was also revealed for the loss of a certain amount of photocatalyst during the experiment.
The detailed morphological features of the Ti0.7W0.3O2/TiO2 NCI were characterized by SEM technology and are shown in Fig. 2(A–D). The pure anatase TiO2 was present as nanospheres, with a uniform size distribution as shown in Fig. 2(A). Fig. 2(B) shows the morphology of the pure rutile Ti0.7W0.3O2 NPs, which were irregular and schistose particles with a smooth surface and highly dense quality. Fig. 2(C) and (D) show that the TiO2 NSs were uniformly dispersed on the surface of the Ti0.7W0.3O2 NPs and formed the Ti0.7W0.3O2/TiO2 NCI.
The elemental composition of the synthesis of the samples was confirmed by EDX spectra. In Fig. 2(a and b), the anatase TiO2 revealed major peaks of Ti and O, and the rutile Ti0.7W0.3O2 NPs revealed major peaks of Ti, W and O. Fig. 2(c and d) evidence the presence of Ti, W and O elements for the Ti0.7W0.3O2/TiO2 NCI, indicating the high purity, and we can easily distinguish between the two components in the composite photocatalyst.47–49
Furthermore, the atomic% of Ti/the atomic% of O of anatase TiO2 was measured as 0.48, which was close to the mol ratio of Ti/O (0.50) in TiO2. The atomic% of Ti/the atomic% of W of rutile Ti0.7W0.3O2 NPs was measured as 2.08, which was close to the mol ratio of Ti/W (2.33) in Ti0.7W0.3O2. The EDX results for each synthesized sample were a little different with the theoretical mol ratio of elements as EDX merely involved a local analysis of the entire surface of samples, and so these represented acceptable errors.50–52
However, the atomic% of Ti/the atomic% of O of anatase TiO2 and the atomic% of Ti/the atomic% of W of rutile Ti0.7W0.3O2 NPs in Ti0.7W0.3O2/TiO2 NCI were measured to be 0.54 and 2.02, respectively. The error of the results had thus increased, which might be due to the interaction between the two nanomaterials.
A UV-Vis spectrometer was used to record diffuse reflectance spectra in the range 200–800 nm. Fig. 3 (A) shows the DRS of pure TiO2 NSs, pure rutile Ti0.7W0.3O2 and 5 wt% Ti0.7W0.3O2/TiO2 NCI. The band gap values of the synthesized photocatalysts were calculated by plotting (F(R∞)hv)1/2versus the photo energy and the plot is shown in Fig. 3 (B). The pure TiO2 NSs and the pure rutile Ti0.7W0.3O2 demonstrated a photoabsorption modification ability for the UV light region with wavelength shorter than 396 and 598 nm, corresponding to band gap energies of 3.21 and 2.05 eV, respectively. The pure rutile Ti0.7W0.3O2 had a shorter band gap energy due to W4+ doped into the lattice of TiO2. When the pure rutile Ti0.7W0.3O2 was irradiated, conduction band electrons (ecb−) were generated and quickly spread to the valence band due to the shorter band gap energy, which might make the semiconductor have higher conductivity.53 The volume resistivity and conductivity of pure anatase TiO2, 0.3 wt% Pt/TiO2 and 5 wt% Ti0.7W0.3O2/TiO2 are shown in Fig. 3(F). The volume resistivity of pure anatase TiO2 was over 10 times that of 5 wt% Ti0.7W0.3O2/TiO2. The volume resistivity of 0.3 wt% Pt/TiO2 was over 2 times that of 5 wt% Ti0.7W0.3O2/TiO2. It was thus indicated that the conductivity of pure anatase TiO2 could be improved greatly by modifying the Ti0.7W0.3O2 NPs, and that the performance of Ti0.7W0.3O2 NPs was superior to that of Pt NPs, which could fully prove the above conjecture.
Meanwhile, the 5 wt% Ti0.7W0.3O2/TiO2 NCI was extended to the visible absorbance region with a wavelength shorter than 527 nm and had a shorter band gap energy of 2.37 eV. The above results were fully proved by ultraviolet photoemission spectroscopy (UPS) and the results are shown in ESI (Section 4, Fig. S7†). The band gap energies of the pure TiO2 NSs and 5 wt% Ti0.7W0.3O2/TiO2 NCI were 3.38 and 2.43 eV, respectively, which were slightly larger than that from the DRS. The reasons for the deviation may be due, on the one hand, to the detection depth of UPS technology, which was 10 atoms, while on the other hand, the carbon pollution signal would be higher for the solid powder sample.
In short, Ti0.7W0.3O2 NPs with higher conductivity can cause fast electron transfer and effectively restrain the recombination of ecb−–hvb+ pairs in Ti0.7W0.3O2/TiO2 NCI, which can diffuse to the surface and react with pollutants and produce more superoxide radical anions (˙O2−)/˙OH−. Furthermore, the Ti0.7W0.3O2/TiO2 NCI could also improve the utilization of visible light, which might account for the higher photocatalytic activity.
The XPS valence band scan spectra of pure anatase TiO2 NSs, rutile Ti0.7W0.3O2 and 5 wt% Ti0.7W0.3O2/TiO2 NCI are shown in Fig. 3(C–E). The valence bands of TiO2 NSs, rutile Ti0.7W0.3O2 and 5 wt% Ti0.7W0.3O2/TiO2 NCI were 3.01, 2.65 and 2.83 eV, respectively. According to the band gap energy result from DRS, the conduction bands were measured as −0.20, 0.60 and 0.46 eV, and the energy level diagram of Ti0.7W0.3O2/TiO2 NCI could be proposed and is shown in ESI (Section 4, Fig. S8†).
The rutile Ti0.7W0.3O2 was further characterized by XPS, as seen in Fig. 4(A–D), to illustrate the structural features and composition. The XPS survey scan spectrum of rutile Ti0.7W0.3O2 is shown in Fig. 4(A). The relative concentrations of Ti and W of Ti0.7W0.3O2 were determined by the respective XPS peak areas and atomic sensitivity factors and nTi/nW was measured as 2.13, which is close to the mol ratio of Ti/W (2.33) in Ti0.7W0.3O254 and consistent with the EDX result.
Fig. 4 XPS survey scan spectra of: (A) rutile Ti0.7W0.3O2, and XPS narrow scans of: (B) O 1s, (C) W 4f and (D) Ti 2p of the rutile Ti0.7W0.3O2. |
The XPS narrow scan spectra of Ti 2p, W 4f and O 1s of the rutile Ti0.7W0.3O2 are shown in Fig. 4(B–D). The Ti 2p1/2 and Ti 2p3/2 peaks of Ti0.7W0.3O2 were located at 464.6 and 458.8 eV and assigned to TiO2, respectively. The W 4f5/2 and W 4f7/2 peaks were located at 34.2 and 33.1 eV, and assigned to WO2, proving that the W6+ was fully reduced to W4+ in Ti0.7W0.3O2.
The most appropriate initial phenol concentration was investigated with the initial concentration ranging from 50–125 ppm and the results are shown in Fig. 5(B). Obviously, the complete photodegradation time of phenol increased with the increase in the initial concentration from 50–95 ppm, and the photodegradation of phenol at 95 ppm could be just finished with 360 min irradiation. The photocatalytic efficiencies of 110 ppm and 125 ppm phenol were 94.3% and 86.3% after 360 min irradiation, respectively. Further increases decreased the photocatalytic efficiency, indicating that there was an optimum value. The reasonable explanations for this are as follows: first, too many phenol molecules and its intermediates would also absorb a part of the irradiation and limit the light absorption capability of the photocatalysts. Second, excessive amounts of phenol molecules and its intermediates also deactivate more active sites and reduce the light penetration to active sites situated on the surfaces of Ti0.7W0.3O2/TiO2 NCI. The above two disadvantages also result in a lower production of superoxide radical anions (˙O2−)/˙OH− and ultimately a lower oxidation ability.57
The effect of the Ti0.7W0.3O2/TiO2 NCI dosage was investigated by varying the dosage from 0.15 g L−1 to 0.90 g L−1 and the results are shown in Fig. 5(C). When raising the Ti0.7W0.3O2/TiO2 NCI dosage from 0.15 g L−1 to 0.60 g L−1, the phenol photocatalytic efficiency increased from 58.7% to 100% as more active sites were available, increasing the response surface area and leading to a greater production of ˙O2−/˙OH−. However, further increasing, the dosage to 0.90 g L−1 decreased the photocatalytic efficiency. According to the literature,58–62 the reasons for this might be due to the following aspects: on the one hand, an excessive dosage of photocatalysts would result in lower solution transparency, light scattering and interception and the prevention of the light induction of some catalysts particles. On the other hand, too many photocatalysts particles would prevent the effective collisions between phenol molecules and a variety of free radicals. Moreover, the pore volume and available surface area of the photocatalysts would also be diminished with excessive dosage, resulting in a lower photocatalytic activity.
The stability and recyclability of all heterogeneous photocatalysts are critically important for application in wastewater treatment plants. The stability and recyclability of Ti0.7W0.3O2/TiO2 NCI were investigated in a batch reactor under pH 4.5, a catalyst dosage of 0.45 g L−1 and phenol concentration of 95 ppm. After each experiment, the used photocatalyst was collected from the suspension turbid solution and washed with 50% ethanol solution to remove residue phenol and other photodegradation products on the photocatalysts surface. Then, the wet photocatalyst was dried at 105 °C for 4 h. This sequence was repeated six times and the phenol photodegradation efficiency of each cycle recorded and the results are shown in Fig. 5(D). After six recycles, the photocatalytic degradation efficiency of Ti0.7W0.3O2/TiO2 NCI was reduced from 100% to 94.5%, indicating that the Ti0.7W0.3O2/TiO2 NCI showed high photocatalytic activity with good stability and recyclability. The reduction could be explained by a loss of photocatalyst during the washing process, which was consistent with the PXRD results.
Fig. 6(A and B) present the phenol photocatalytic degradation by P-25, Pt/TiO2 and Ti0.7W0.3O2/TiO2 NCI, showing the differences in the phenol degradation activity with the varying loading rates of Ti0.7W0.3O2/TiO2 and Pt/TiO2. The phenol degradation rate of Ti0.7W0.3O2/TiO2 NCI increased with the loading value of Ti0.7W0.3O2 up to 5 wt%; however, a further increase would decrease the photocatalytic activity, indicating that there was an optimum loading value. The optimum value had a close relationship with the dispersion and particle sizes of Ti0.7W0.3O2 NPs. Meanwhile, one could easily find that the phenol degradation rate of 5 wt% Ti0.7W0.3O2/TiO2 NCI was always higher than that of 0.3 wt% Pt/TiO2 at any synchronous irradiation time, revealing its higher photocatalytic activity.
Fig. 6(C and D) compare the phenol photocatalytic degradation rates of P-25, Pt/TiO2 and Ti0.7W0.3O2/TiO2 NCI after 360 min irradiation. The phenol photocatalytic degradation rate after various intervals of time was estimated using the following eqn (2).
Phenol photocatalytic degradation rate (%) = (ct=0 − ct)/ct=0 × 100% | (2) |
Fig. 7 Dependence of In (c0/c) on the irradiation time (t) for: (A) Ti0.7W0.3O2/TiO2 NCI, (B) P25 and Pt/TiO2. |
The initial rate constant (k) for phenol photocatalytic degradation in P-25 was calculated as 0.00346 min−1, while the initial rate constant (k) for phenol photocatalytic degradation in 5 wt% Ti0.7W0.3O2/TiO2 and 0.3 wt% Pt/TiO2 was about 26 and 6.8 times that of P-25, respectively. This indicated that the photocatalytic activity of TiO2 was enormously improved with the proper amount of loading Ti0.7W0.3O2 and Pt NPs. Furthermore, the initial rate constant (k) for 5 wt% Ti0.7W0.3O2/TiO2 was over 3.9 times that in 0.3 wt% Pt/TiO2, illustrating that the as-prepared Ti0.7W0.3O2 NPs may be much superior to Pt NPs in embellishing the photocatalytic properties of TiO2 nanomaterials and could even replace them.
Herein, to better assess the photocatalytic activity of the synthesized Ti0.7W0.3O2/TiO2 NCI, we compared our results with the photodegradation of phenol reported in previous studies, as shown in Table 1. The Ti0.7W0.3O2/TiO2 NCI showed several advantages in the photocatalytic performance, photocatalytically degrading the most amount of phenol with the least irradiation time and catalyst dosage. The initial rate constant (k) of the Ti0.7W0.3O2/TiO2 NCI was over 2.6 times that of SnS2/TiO2 nanocomposite catalyst, which showed a higher photocatalytic activity than the other catalysts. Therefore, it was concluded that the Ti0.7W0.3O2/TiO2 NCI was one of the most efficient catalysts for the photocatalytic degradation of phenol under the selected experimental parameters.
Catalyst | Concentration (mg L−1)/volume (mL) of phenol | Catalyst amount (g L−1) | Degradation (%) | Irradiation time (min) | Initial rate constant (k) (min−1) | Reference |
---|---|---|---|---|---|---|
Pt–ZnO | 15 | — | >95 | 540 | — | 63 |
ZnO | 50/200 | 1.0 | 69.75 | 480 | 0.0150 | 64 |
GO/TiO2 | 14/100 | 1.48 | 100 | 180 | — | 65 |
RGO/TiO2 | 50/1700 | — | 96 | 180 | 0.0154 | 66 |
MWCNT/TiO2 | 50/800 | 1.0 | 96 | 300 | 0.0074 | 67 |
Fe/S/TiO2 | 20/60 | 1.0 | 99.4 | 600 | — | 68 |
CNT/Ce–TiO2 | 50/500 | 0.4 | 95 | 180 | 0.0012 | 69 |
BiPO4 | 50/100 | 0.5 | 100 | 240 | 0.0370 | 70 |
Co/Pd/BiVO4 | 18.4/100 | 0.8 | 90 | 180 | 0.0130 | 71 |
ZnO/TiO2 | 60/250 | 0.6 | 100 | 160 | 0.0124 | 72 |
TiO2−xBx | 94/50 | 6 | 97 | 240 | 0.0084 | 73 |
BiMnO4 | 20/100 | 1.0 | 90 | 480 | 0.0049 | 74 |
Fe(III)–TiO2 | 100/1500 | 0.5 | 93.8 | 210 | 0.0190 | 75 |
TiO2/Ag/C | 20/100 | 1.0 | 95 | 60 | — | 76 |
N–TiO2@CS | 9.4/40 | 2.5 | 90 | 180 | — | 77 |
V2O5/N,S–TiO2 | 100/20 | 1.0 | 88 | 240 | — | 78 |
Pt/TiO2 | — | — | 87.7 | 180 | — | 79 |
TiO2–Fe2O3–graphene | 5/100 | 1.5 | — | 150 | 0.01415 | 80 |
SnS2/TiO2 | 10/100 | 0.5 | — | 150 | 0.03595 | 81 |
Ti 0.7 W 0.3 O 2 /TiO 2 NCI | 95/1000 | 0.45 | 98.7 | 50 | 0.09111 | This study |
The UV-Vis absorption spectra from the photodegradation of phenol over P-25, Pt/TiO2 and Ti0.7W0.3O2/TiO2 are compared in ESI (Section 6, Fig. S10†). At P-25, besides the characteristic absorption bands at 270 nm of phenol, a new absorption band at 289 nm appeared, which might be attributed to the ring-retaining compounds.29,59,86,87 However, besides the two absorption bands at 270 and 289 nm, there were two new absorption bands at 247 and 257 nm for Pt/TiO2, and another two new absorption bands at 333 and 363 nm for Ti0.7W0.3O2/TiO2, which might be attributed to ring-opened produciits.87,88 It can be concluded that the phenol photodegradation pathway over Ti0.7W0.3O2/TiO2 NCI was partially different from that over P-25 and Pt/TiO2.
The aqueous solutions of phenol degradation over P25, Pt/TiO2 and Ti0.7W0.3O2/TiO2 were detected by UV-Vis spectrometry, UHPLC-MS and GC-MS. Then, the main intermediates were analyzed and inferred by the molecular ions and mass fragment peaks present and from library data. The LC chromatograms, UV-Vis spectrograms and mass spectra from HPLC-MS are shown in ESI (Section 7, Fig. S11a–k†). The GC chromatograms and mass spectra from GC-MS of the intermediates are shown in ESI (Section 8, Fig. S12 and S13†). The analytical results and possible structures of each intermediate are shown in ESI (Section 9, Table S1 and Fig. S14†).
In short, five and six kinds of intermediates were identified in the aqueous suspension of P-25 and Pt/TiO2, respectively. Six kinds of intermediates were found in the aqueous suspension of Ti0.7W0.3O2/TiO2. The further degradation of all the intermediates might include oxidative hydroxylation and oxidative decarboxylation products, etc. from several reaction pathways operating simultaneously.
Figure 8(B) presents the fluorescence intensity as a function of the duration of irradiation. The fluorescence intensity increased linearly with the irradiation time, showing that the formation superoxide radical follows the quasi-first-order-type kinetics, as evidenced by the linear relationship between the concentration of superoxide radical and irradiation time within a certain range.
Therefore, based on the present experimental data and the referenced studies,29,59,91,94–97 the different intermediates of P-25, Pt/TiO2 and Ti0.7W0.3O2/TiO2 indicate the different phenol degradation processes, as clearly illustrated in Fig. 9.
Fig. 9 Proposed photocatalytic degradation process of phenol over: (A) P-25, (B) Pt/TiO2 and (C) Ti0.7W0.3O2/TiO2 NCI. |
In addition, we believe that the photocatalytic degradation of phenol over P-25 follows a radical reaction mechanism. The photocatalytic degradation of phenol over Pt/TiO2 and Ti0.7W0.3O2/TiO2 follows both a radical reaction mechanism and holes reaction mechanism, which proceed in parallel.
The phenol photocatalytic degradation mechanism involves initial reactions at the Ti0.7W0.3O2/TiO2 NCI, as shown in Scheme 1. It was well established that conduction band electrons (ecb−) and valence band holes (hvb+) were generated when the suspension was irradiated. A Schottky barrier might be formed at the NCI between TiO2 NSs and Ti0.7W0.3O2 NPs, leading to a greater formation of hvb+ and ecb− and an enhanced photocatalytic activity.59 Ti0.7W0.3O2 NPs with high conductivity might cause fast electron transfer and effectively restrain the recombination of ecb−–hvb+ pairs in the bulk catalyst, which can then diffuse to the surface and react with pollutants.54 Hydroxyl radical (˙OH−) formation occurred at the Ti0.7W0.3O2/TiO2 NCI by hvb+ trapping absorbed hydroxyl and hydration molecules (OH−/H2O). Meanwhile, ecb− could react with molecular oxygen (O2) adsorbed at the NCI and produce superoxide radical anion (˙O2−). Acidic conditions could generate a higher affinity towards unpaired ecb− of NCI, leading to the formation of more hydroxyl radicals (˙HO2−).98,99 The hvb+ could also oxidize pollutants directly. These might account for the extraordinary photocatalytic activity of Ti0.7W0.3O2/TiO2 NCI.
Footnote |
† Electronic supplementary information (ESI) available: The synthesis and characterization of Pt/TiO2 nanocomposite; the detail information of characterization, photocatalytic test and analysis of intermediates of photocatalytic degradation of phenol; particle size analysis; the Ultraviolet Photoemission Spectroscopy (UPS) analysis; the UV-Vis spectra of phenol degradation catalyzed by P-25, Pt/TiO2 and Ti0.7W0.3O2/TiO2 NCI; compared the characteristic UV-Vis spectra of phenol degradation intermediates; the LC chromatogram, UV-Vis spectrogram and mass spectrum of main intermediates; the UV-Vis absorption spectra, GC chromatogram and mass spectrum of GC-MS for intermediates; the analysis result and possible structure of each intermediate. See DOI: 10.1039/c9na00478e |
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