Abstract
The hydrothermal method was used to synthesize carbon sphere, and the hard template synthesis method was used to prepared C-doped hollow TiO2 sphere (CHTS). Bismuth nitrate was used as bismuth source to modify CHTS. The composite material was oxidized in air atmosphere at 450℃ to obtain Bi2O3 modified C-doped TiO2 hollow spheres(BCHTS). The morphology, elemental composition and photocatalytic degradation efficiency of tetracyclines (TC) by BCHTS hollow spheres were characterized by various measurements. Additionally, the possible transformation pathways and degradation mechanism of tetracycline were revealed via LC–MS and trapping experiments. The experimental results show that the Bi nanoparticles are uniformly dispersed in the CHTS. The photocatalyst exhibits enhanced degradation rate of TC (98.4% under visible-light within 180 min and 99.4% under natural light within 50 min) for its structure and narrow bandgap (2.87 eV). After five degradation cycles, the photocatalyst still remains high removal rate of 96.4% for TC. The results indicate that the photocatalyst may be promising for degrading antibiotic residuals remains. According to the trapping experiment, OH and h+ have a certain role on the photodegradation process, while·O2− is the main active species for degrading TC.
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1 Introduction
In recent years, antibiotics have been widely used not only in human medical care, but also in aquaculture and animal husbandry for medical and non-medical enhanced crop production. However, the overuse of antibiotics causes their residues to be widely dispersed in the environment, posing a serious threat to human and ecosystem health [1, 2]. Therefore, the development of effective methods to degrade or remove antibiotic residues from the aquatic environment is critical.
At present, these current methods can be loosely classified into three types: physical removal (adsorption, sedimentation, flocculation and filtration) [3, 4], biological treatment [5, 6] and chemical degradation (ozonation, chlorination, and Fenton’s oxidation) [7,8,9]. Alternatively, photocatalysis is gaining increasing global interest and is widely implemented in new energy extraction and environmental control strategies with substantial progress made in recent years [10, 11]. Cai [12] found that Cr3+ doping SrTiO3 cubic nanoparticles could only degrade 70% of tetracycline (TC) under visible light. Zhang [13] prepared Ce3+ doped Bi2O3 hollow needle-shape with removal rate of 89% for TC. Additionally, Wang [14] realized the degradation 94% of TC over Bi3+ doped ultrathin g-C3N4 nanosheets under visible light. However, it is still a big challenge to further improve the degradation efficiency of photocatalyst for antibiotics under visible light.
For a long time, TiO2 has attracted much attention as a photocatalytic material due to its advantages of good photochemical stability, non-toxicity, photocatalytic activity and low cost [15]. However, the broadband gap results in that TiO2 can only absorb ultraviolet light (4% of the solar spectrum) [16, 17].
In order to further improve the photocatalytic activity of TiO2, researchers have tried various methods. From the perspective of structure, hollow spherical nanostructures can make light reflect and scatter multiple times within the shell, thus extending the path of light to enhance the absorption capability [18,19,20,21,22]. Appropriate doping of metallic or nonmetallic elements can produce intermediate energy levels within the band gap, providing a springboard for electron conversion, which allows low-energy photons to be adsorbed to longer wavelengths, thus extending the range of light absorption. Carbon doping exhibits considerable potential advantages over non-metal doping. Firstly, carbon presents metallic conductivity [23]. Secondly, carbon has a large electron-storage capacity and can accept the photon-excited electrons to enhance the separation of photo-generated carries [24]. More particularly, carbon element is always indicated permeating to the lattice of TiO2 and forms O–Ti–C bond in the process of doping, which produces a hybrid orbital above the valence band of TiO2 and extends the visible-light absorption [25]. On the other hand, α-Bi2O3 has superior visible light absorption capacity for its band gap of 2.85 eV and dye sensitization effect [26, 27]. However, pure Bi2O3 photocatalyst has some problems such as poor structural stability and the fast recombination of photogenerated charge carriers, which limits the application of Bi2O3 in photocatalysis [28, 29]. To address the problem, C-doped hollow TiO2 sphere with stable structure was used as primary catalyst and Bi2O3 nanoparticles was used as cocatalyst, respectively.
Though the C-doped TiO2 or Bi2O3/TiO2 composites were prepared and studied by some research workers [30,31,32], there are no report about Bi2O3 modified C-doped TiO2. In this paper, the carbon spheres were prepared by glucose hydrothermal method as substrate, and C-doped TiO2 hollow spheres were prepared by template sacrifice method. The prepared C-doped TiO2 hollow spheres were used to adsorb Bi3+, and Bi3+ was oxidized to Bi2O3 by calcination in air environment at 450℃. Finally, C-doped TiO2 hollow spheres modified by Bi2O3 were obtained. The composite has excellent photocatalytic activity for its outstanding redox capability, visible-light absorption ability.
2 Experimental Section
2.1 Materials
Glucose anhydrous (C6H12O6, AR), hexadecetyltrimethyl ammonium bromide (CTAB, AR), tetrabutyl titanate (TBOT, CP), bismuth nitrate [Bi(NO3)3)•5H2O, AR], bismuth oxide(Bi2O3, AR), ethanol (C2H5OH, AR), and tetracyclines (TC, CP) were purchased from Sinopharm Corporation Ltd. (Shanghai, China). 0.04 M dilute nitric acid was prepared with nitric acid (HNO3 at 68%, CP) purchased from Sinopharm Corporation Ltd. Deionized water was employed in all experiments. All chemicals were used without further purification.
2.2 Experimental
2.2.1 Preparation of Carbon Sphere Templates
In a typical procedure [33,34,35], 14.4 g of glucose was firstly dissolved in deionized water (80 mL). Then the solution was transferred into a 100 mL Teflon-lined stainless steel autoclave. Finally, hydrothermal treatments were carried out at 240 ℃ for 4 h and then cooled down to room temperature naturally. The obtained products were filtered and washed with alcohol and deionized water for several times, then dried at 60 ℃ for 12 h.
2.2.2 Preparation of C-doped TiO2 Hollow Spheres
The prepared carbon spheres (0.4 g) were firstly dispersed in ethanol (30 mL). The cetyltrimethyl ammonium bromide (CTAB, 0.2 g) was dissolved in 70 mL ethanol and 0.4 mL deionized water mixture solution, and then the prepared carbon spheres solution was added into the CTAB solution. After stirring 2 h, tetrabutyl titanate (TBOT, 2 mL) in ethanol (20 mL) was injected by dropping. Subsequently, the solution was stirred for 24 h at room temperature. The final products were centrifuged and washed with ethanol and dried at 60 ℃ for 10 h. In addition, the product was calcined at 450 ℃ for 2 h to remove the carbon sphere. The sample was denoted as CHTS. For comparison, the TiO2 nanoparticles (TNP) were prepared without carbon sphere addition by the same process.
2.2.3 Preparation of Bi2O3 Modified C-doped TiO2 Hollow Spheres
The prepared CHTS (50 mg) was dispersed in 50 mL ethanol, and 10 mL HNO3 (0.04 M) mixed with Bi(NO3)3·5H2O (20 mg) was added into the solution and stirred for 2 h. Subsequently, the solution was stirred at 60 ℃ until it was evaporated. The products were calcined at 450 ℃ for 2 h. The sample was denoted as BCHTS. The whole prepare process is shown in Fig. 1.
2.3 Characterization
The crystal structure and composition were carried out on a D8 ADVANCE powder X-ray diffractometer (XRD), and a scanning rate of 5°/min was used to record the patterns in the 2 theta angle ranging from 5° to 90°. JEM-2100(HR) transmission electron microscope (TEM) and FEI NovaNano450 scanning electron microscope (SEM) were used to characterize the morphology of the samples. The elemental composition was tested on a Thermo Scientific K-Alpha X-ray photoelectron spectrometer (XPS). Identification of the intermediates in the photodegradation of TC was analyzed by a liquid chromatography–mass spectrometry (LC–MS, Thermo LXQ LC/MS), and the mass range is from m/z 50 to 600.
2.4 Photocatalytic Activity Measurements
The photocatalytic activity of the catalysts was evaluated by the degradation of tetracyclines (TC) under visible light irradiation. A 300 W Xenon lamp was used as the simulated solar light. The 420 nm cut off filter was used to get the visible light source. In each experiment, 10 mg of the as-prepared photocatalyst was added into 50 mL tetracyclines solution (10 mg/L). Before irradiation, the suspensions were placed in dark and stirred for 30 min to ensure the establishment of adsorption–desorption equilibrium between the catalyst and tetracyclines. Subsequently, at every interval, about 3 mL suspension was sampled and centrifuged to remove the photocatalyst particles. The concentration of filtrates was analyzed by measuring the maximum absorbance at 357 nm for tetracyclines using a UV-2600 UV–vis spectrophotometer.
The degradation rate of the catalyst to the dye can be expressed as:
In the formula (1), C0 represents the initial concentration (mg/L) of the TC solution, and C represents the current concentration (mg/L) of the TC solution measured at the time of sampling.
3 Results and Discussion
3.1 SEM and TEM Analyses
SEM images of CS, CHTS and BCHTS are shown in Fig. 2. The prepared carbon sphere template (Fig. 2a) is smooth and regular spherical shape, and the carbon spheres are connected with each other by some degree of adhesion, while the diameter of the sphere is about 500–720 nm. After coating the surface of the carbon spheres with a layer of TiO2 and removing the template of the carbon spheres (Fig. 2b), the surface of the sample become rough, and the diameter is increased to about 550–780 nm, which indicates that TiO2 is successfully coated on the surface of the carbon spheres with a thickness of about 50 nm. At the same time, some broken spheres can be seen in Fig. 2b, which indicates that the template of the carbon spheres has been removed, and the catalyst prepared is a hollow spherical structure. After loading Bi2O3 (Fig. 2c), the diameter and morphology of the catalyst do not change greatly, while the surface becomes more rough, and there are many raised small particles, indicating that Bi2O3 is loaded on the C-doped TiO2 hollow sphere in the form of nanoparticles. In addition, there are some fine nanoparticles, which may be caused by the collapse of some structures due to calcination of the catalyst. Figure 2d shows the TEM image of BCHTS. It can be further seen that the catalyst is a piece of interconnected hollow spherical structure. The HRTEM (Fig. 2e) shows that BCHTS consists of α-Bi2O3 with lattice spacing of 0.239 nm (112)[36] and anatase TiO2 with lattice spacing of 0.352 nm (101)[37], which reveals the successive coupling of TiO2 and Bi2O3. Meanwhile, SEM mapping of BCHTS in Fig. 2f-j indicates that BCHTS contains Ti, O, Bi and C elements. Bi signal is evenly distributed in the sample (Fig. 2i), and some C elements are doped in the sample during the removal of the hard template (Fig. 2j).
3.2 XPS and XRD Spectra
The XPS survey spectrum of BCHTS confirms the existence of Ti, O and Bi (Fig. 3a). As shown in Fig. 3b, Ti 2p spectrum of BCHTS is observed, and the binding energy of Ti 2p are 458.3 eV (2p3/2) and 464.0 eV (2p1/3)[38]. Besides, the XPS spectra of O 1 s can be fitted into two peaks at 529.5 eV and 531.0 eV (Fig. 3c). The peak at 529.5 eV is attributed to the lattice oxygen, while the latter one is assigned to the defect sites with a low oxygen coordination. This may suggest the generation of oxygen vacancies [39, 40]. For Fig. 3d, we find four broad peaks in the Bi 4f spectrum. Two prominent peaks at 158.9 eV and 164.2 eV are ascribed to characteristic arbital splitting of Bi 4f7/2 and Bi 4f5/2, respectively, while two peaks at 157.2 eV and 162.7 eV are attributed to metallic Bi0 [41]. This may suggest that some of Bi3+ were reduced at the process of preparation. There are three peaks in the C 1 s spectrum (Fig. 3e). The peaks at 285.8 eV and 288.2 eV are characteristic peaks of the oxygen bound species C–O and C-Ti–O, respectively. These indicate that carbon elements are always indicated permeating to the lattice of TiO2 and form O–Ti–C bond in the process of doping [42].
The XRD patterns of CHTS and BCHTS are described in Fig. 3f. The peaks of CHTS at values of 25.3, 38.0, 48.0, 53.7, 55.0 and 62.5°are respectively attributed to (101), (004), (200), (105), (211) and (204) crystal planes of typical TiO2[43]. All peaks are indexed to the anatase of TiO2 (JCPDS: 21–1272). Meanwhile, some peaks of BCHTS well correspond to the standard of anatase, and the other characteristic diffraction peaks can also be indexed to the Bi2O2.33 (JCPDS: 27–0051)[44]. This suggests that part of Bi0 are contained in the sample apart from Bi2O3. All results are consistent with XPS spectrum, which further proves that Bi is uniformly dispersed in the sample.
3.3 UV–Vis Analysis
The light-harvesting capability and the corresponding forbidden bandwidth obtained by Kubelka–Munk model of CHTS and BCHTS were analyzed via UV–Vis absorption spectra. As shown in Fig. 4a, besides strong UV light absorption, BCHTS exhibits a weak visible light absorption than CHTS. According to the Kubelka–Munk model (Fig. 4b), the bandgap of CHTS (3.12 eV) is similar to anatase (3.2 eV). Meanwhile, BCHTS shortens its bandgap from 3.12 to 2.87 eV after modified by Bi2O3. This result show that BCHTS is more prone to be excited under visible light due to its more narrow forbidden bandwidth [45].
3.4 Photocatalytic Performance
The photocatalytic performance of BCHTS was investigated by degrading TC which was widely used as contaminants under visible-light. As shown in Fig. 5a, the obvious absorption peak of TC can be observed at value of 357 nm. After stirred for 30 min in the darkness, the absorption peak of TC just becomes lower without any changes, and the characteristic peak (357 nm) is gradually decreased and disappeared when TC is illuminated under visible-light. This suggests that the prepared BCHTS can efficiently degrade TC under visible-light. The photocatalytic performance of BCHTS under different lights is shown in Fig. 5c. The degradation of TC is almost unchanged after stirring for 30 min in the darkness, which indicates that the absorption equilibrium is achieved after only 30 min stirring. The TC is degraded completely after 50 min under natural light. Meanwhile, to better evaluate the photocatalytic activity, Bi2O3, CHTS, and TNP were used as reference samples (Fig. 5d). Under visible-light irradiation, the degradation rates of TC are only about 32.2% and 79.7% within 180 min for Bi2O3 and TNP, respectively. Compared to them, the degradation of TC for CHTS and BCHTS can reach 89.9% and 98.4% within 180 min under visible-light, which well manifest that both the hollow sphere structure and the modification of Bi2O3 have great effects on the improvement of the photocatalytic performance of TiO2. Specially, the removal of TC almost come up to 100% with the help of BCHTS under visible light, which is higher than the photocatalysts in previous researches [12,13,14, 46].
3.5 Possible Transformation Pathways of TC
In order to identify the potential structure of photodegradation products, the MS determination was performed. The MS spectra of TC degradation solution after 100 and 180 min irradiation can be seen in Fig. 6, which reveals the occurrence of several peaks and attributes to the photodegradation products with m/z values of 475, 461, 438, 415, 393, 349, 361, 305, 242, 210 and 175. Based on the photodegradation intermediate products, the transformation pathway is proposed as shown in Fig. 7, which can be outlined by three routes.
During the whole transformation process, the intermediates are mainly generated by two routes with the loss of functional groups and the open-ring reactions. For pathwayI, the TC 1 (m/z = 445) are attacked by reactive oxygen species to the double bond to obtain the oxidative compound TC 2 (m/z = 461). Then, TC 3 (m/z = 349) was formed during the deamination reaction, the breaking and oxidation of the ester bond, the carbon–carbon double bond and the ring. As the photodegradation is progressed, the ring opening reactions and the oxidative decomposition are further occurred to form TC 4 (m/z = 305) and TC 5 (m/z = 261) [47]. For pathway II, TC 6 (m/z = 475) is formed from the addition reaction, the rearrangement with the ·OH radicals and the oxidation of N-methyl to N-aldehyde group. Then TC 6 might be transferred to TC 7 (m/z = 438) through dislodging N–C bond and hydroxyl-substitution reaction by the attack of ·OH radicals. TC 7 is transferred into TC 8 (m/z = 210) via the loss of methyl and hydroxyl group and the rupture of C–C single bond leading to the breakage of ring [48]. For pathway III, TC 1 is first transformed into TC 9 (m/z = 415) which is also proved by other researches [49, 50]. The TC 10 (m/z = 393) is generated from TC 9 by the dealkylation, deamination and dehydration process. Then TC 11 (m/z = 242) and TC 12 (m/z = 175) are formed via ring-opening process [51].
3.6 Photodegradation cycle of TC
The reusability of photocatalysts are crucial for the potential application in wastewater disposal. Therefore, the cycle experiment was conducted over BCHTS toward the degradation of TC. After each test, the photocatalyst was filtrated, washed and finally dried at 60 °C for 12 h. Figure 8a and Fig. 8b show that after five photodegradation cycles of TC, the degradation rate of TC still remains 96.4%, which indicates that the degradation activity of BCHTS is almost excellent even after five degradation processes. This suggests that the prepared BCHTS photocatalyst has superior reusability. Notably, XRD test (Fig. 8c) shows that the crystal structure of BCHTS remains unchanged after five cycles, which indicates that BCHTS has excellent stability and sustainability of structure. This is the reason for the superior cycling performance of BCHTS.
3.7 Trapping Experiment
To learn more photodegradation mechanism of TC, the role of active species was investigated via trapping experiment. Nitrogen, isopropyl alcohol (IPA) and triethanolamine (TEA) were employed to quench·O2−, ·OH and h+, respectively. When N2 is pumped into the reaction system, the generation of ·O2− is limited by the absence of O2. Different from the restraints of ·O2− by N2, ·OH and holes are restrained by quench technique. The principle of this method is that active species can be quenched by certain substances, and cannot play their original role. The specific experimental method is to add a specific quenching agent (sometimes called scavenger) in the photocatalytic degradation process. When the active species were restrained, we can observe whether the removal of pollutants is lower. If the removal is lower, it indicates that the contribution of the active species in the degradation process is higher. Figure 9a and Fig. 9b show that the addition of IPA and TEA makes the degradation of TC reduce to 92.4%, which reveals that ·OH radicals and h+ play a certain role during the photodegradation process. While bubbling N2 greatly suppresses the removal of TC to 85.2%, indicating that ·O2− radicals are the main active species for degrading TC under visible light irradiation [52,53,54].
4 Conclusions
To obtain enhanced photocatalytic activity under visible-light, the carbon spheres were prepared by hydrothermal process with glucose, and Bi2O3 modified C-doped TiO2 hollow spheres were prepared by sol–gel method based on carbon spheres with subsequent deposition–precipitation and calcination under air atmosphere. The prepared hollow structured photocatalysts with diameter about 500–720 nm and shell thickness of 50 nm show highly efficient visible light induced photocatalytic activities. The degradation rates of TC reach 98.4% under visible-light within 180 min and 99.4% under natural light within 50 min, respectively. Besides, the BCHTS exhibits good stability even after five cycles. After five cycles, it still remains high removal of TC with degradation rate of 96.4%. Additionally, the possible transformation pathways and degradation mechanism of tetracycline were revealed via LC–MS and trapping experiments in this paper. The prepared hollow structured photocatalyst may be a promising photocatalyst for degrading organic pollutants and environmental remediation.
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Acknowledgements
The work was supported by National Natural Science Foundation of China(No. 20207003, No. 20704019, No. 51603093), Innovative and Entrepreneurial Building Team Project of Jiangsu Province(No. 2015026) and New Green Materials Project of Hangmo New Materials Group Co., Ltd.. The authors wish to express their appreciation to the Analytical Center at Jiangsu University for the measurements of samples.
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Chai, F., Meng, F., Liu, S. et al. A Novel Bi2O3 Modified C-doped Hollow TiO2 Sphere Based on Glucose-derived Carbon Sphere with Enhanced Visible Light Photocatalytic Activity. J Inorg Organomet Polym 32, 2298–2308 (2022). https://doi.org/10.1007/s10904-022-02291-3
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DOI: https://doi.org/10.1007/s10904-022-02291-3