Guangda Xiaa,
Sichen Xiaoa,
Junjie Sua,
Hui Zhoua,
Yu Liu*a and
Xiaodong Zhub
aCollege of Material Science and Engineering, Northeast Forestry University, Harbin 150040, China. E-mail: liuyu820524@126.com
bKey Laboratory of Bio-based Material Science and Technology (Northeast Forestry University), Ministry of Education, Harbin 150040, China
First published on 11th January 2023
A large quantity of wastewater is released from wood processing, posing a serious pollution problem to the natural environment. Photocatalysis has become a reliable method for effluent purification. In this paper, balsa-templated BiVO4–CdS (BBC) was synthesized by impregnation calcination and chemical deposition using wood residue as a template. Rhodamine B (RhB) is used as a wood colorant and is present in wood processing wastewater. The performance of BBC in photocatalytic degradation with simultaneous hydrogen production was identified using RhB as simulated wood dye wastewater and a sacrificial electron donor. Compared to the BiVO4–CdS without a template, the BBC exhibited higher photocatalytic degradation performance (98.32%), which was attributed to the laminar porous structure of the wood being replicated. Because of the existence of a porous structure, BBC has better adsorption properties, which accelerated photodegradation and the production process of H2. Furthermore, surface modification with CdS nanoparticles formed Z-scheme heterojunctions, which greatly inhibited the photogenerated electron–hole compounds. When RhB provided electrons to BiVO4 and CdS, it was also removed by the oxidation of h+ and ·OH, which were simultaneously generated by balsa-templated BiVO4–CdS. BBC produced hydrogen at a higher rate (61.2 μmol g−1 h−1), realizing dual-functional photocatalysis. Therefore, the results support further development of dual-functional catalysts by the use of wood residues.
Currently, BiVO4 has become an important material in photocatalytic remediation of the environment due to its narrow bandgap and strong visible light response.9 However, its practical application in photocatalytic treatment is limited by its poor adsorption performance and the tendency of photoexcited carriers to compound.10,11 CdS is widely used as a hybrid element for semiconductor compounding.12,13 However, the coupling of the two still suffers from the lack of capacity to adsorb for pollutant molecules.14
Plenty of reports declare that different micromorphologies affect the adsorption properties of BiVO4.15 For example, BiVO4 artificial leaves that replicate the unique leaf-like morphology16 and corn straw templates of BiVO4 (ref. 17) exhibited stronger adsorption capacity than that of pure BiVO4. Inheriting the microstructure of natural materials is a way to modify the micromorphology of photocatalytic materials. However, high costs and complicated processes limit the majority template catalysts out of the laboratory and applied in large-scale practical production. Therefore, in a practical production sense, it is considerable to design and search for economical and sustainable materials as templates. In the natural world, wood is abundant and has a complex and regular layered porous structure, including nanoscale molecular fibres, micron-scale transverse rays, and millimetre-scale ductal pores. These factors make wood a good photocatalytic biomimetic template.18–20 However, plenty of wood processing residues are generated in the production and processing every year, with sawmill residues ranging from 35 to 45% depending on moisture content, wood species, log size, and production equipment; fibreboard or oriented strandboard production accounts for 4–12% of wood processing residues, with edge trimming of plywood and splicing of blockboard resulting in an increase of wood processing residues (45%); and approximately 40–50% of the input wood material can be recovered as useable fibre in the pulp manufacturing process.21,22 Hence, by using wood processing residues as a template to prepare photocatalysts for treating wood dyeing wastewater, the waste of valuable wood resources will be reduced.
In this study, a BiVO4–CdS catalyst with a balsa wood was obtained by impregnation-calcination and chemical deposition. The dual-functional of balsa-templated BiVO4–CdS were investigated through the removal and synergistic H2 production of RhB. Finally, the photogenerated electron–holes migration mode and principle of photocatalysis in balsa-templated BiVO4–CdS were clarified by trapping experiments and energy band analysis. This work provides a promising approach for the development of dual-functional biomass-templated photocatalysts.
To set up control samples, BiVO4, CdS, and BiVO4–CdS (1:2) (without template) were prepared. The BiVO4 precursor solution (as described in Section 2.2.1) was dried at 80 °C for 48 h in a drying oven. Then solid residues were calcined at 600 °C for 6 h. BiVO4 was successfully obtained. Cd(CH3COO)2·2H2O (1 mmol) was dissolved in 50 ml of deionized water. Then 10 ml of 0.1 mol L−1 CH4N2S was dipped into the above liquid with vigorous stirring for 20 min. After the mixture was heated at 90 °C for 2.5 h and placed in a dark location for 24 h, the obtained samples were collected by centrifugation and rinsed with anhydrous ethanol and deionized water, then dried at 70 °C for 12 h. CdS was successfully obtained. BiVO4–CdS (1:2) (without template) was labeled as BC.
Fig. 2 (a) XRD patterns of the prepared catalysts and (b) XRD patterns of BC, BBC-1, BBC-2, BBC-3, and BBC-4 with 2θ of 25–28°. |
The chemical binding conditions of BiVO4 and CdS can be identified by XPS. The XPS spectrum of BBC (Fig. 3a) shows that Cd, S, Bi, V, and O are the main elements of BBC. Bi3+ in BiVO4 (Fig. 3b) is observed with two high peaks at 158.58 eV (Bi 4f 7/2) and 163.88 eV (Bi 4f 5/2).26 Compared to both, the XPS peaks of Bi 4f in BBC are shifted to 158.28 eV and 163.48 eV. The XPS signal of O 1s in BiVO4 (Fig. 3d) is found at characteristic peaks of 529.28 eV and 531.38 eV. The binding energies of O 1s in BBC are shifted to 529.18 eV and 531.58 eV, respectively, which represent lattice oxygen and surface-adsorbed oxygen.27 After replicating the microstructure of balsa wood, the adsorption capacity of BBC on dissolved oxygen was greatly improved, which was reflected in the peak intensity of BBC increased at 531.58 eV. The positions of the characteristic peaks of Bi, V, and O demonstrate the successful synthesis of the monoclinic BiVO4. The peaks of Cd2+ in CdS (Fig. 3e) are 404.98 eV and 411.68 eV (Cd 3d 5/2). The Cd 3d in BBC shifts to 404.78 eV and 411.48 eV, respectively.28 The XPS pattern of Cd and S indicate that hexagonal CdS was uniformly loaded on the BiVO4 surface.29 Additionally, the positive shift of the characteristic peaks of V 2p (Fig. 3c) in BBC and the shift of the characteristic peaks of Bi 4f, S 2p, and Cd 3d to lower energies indicate the effective chemical interaction and good binding between BiVO4 and CdS,30,31 which is consistent with the XRD results.
Fig. 3 Survey XPS spectra (a) and high-resolution XPS spectra of Bi 4f, S 2p (b), V 2p (c), O 1s (d), Cd 3d (e) and C 1s (f). |
The inheriting of wood microstructure in BiVO4 was studied by SEM. By replicating the microscopic morphology of the wood (Fig. 4b and c), BiVO4–CdS changed from the original irregular arrangement (Fig. 4a) to a tubular organization with a diameter of approximately 7–15 μm, growing along the longitudinal wood ray cavities of the wood. When balsa wood samples were impregnated in BiVO4 precursor solution, plenty of the solution entered the wood cells and occupied the space along the wood ray channels (Fig. S1†); thus, most of the internal structure of the wood was preserved after calcination. In addition, CdS nanoparticles are uniformly bound to the surface of BiVO4 by the high magnification SEM images. The EDS data (Fig. 4e) demonstrates the presence of Bi, V, O, Cd, and S elements in BBC, while CdS is modified on BiVO4, which is consistent with the XPS results. The HRTEM image of BBC (Fig. 4d) shows that the lattice spacing of 0.31 nm corresponds to the (121) crystal plane of monoclinic phase BiVO4,32 while the lattice spacing of 0.32 nm corresponds to the (101) crystal plane of the hexagonal phase CdS. The TEM results further confirm the good binding of BiVO4 and CdS.29
Fig. 4 SEM images of BiVO4 (a), BC (b), and BBC-3 (c); TEM image and HRTEM image of BBC-3 (d); EDS pattern and elemental mapping of BBC-3 (e). |
The pore condition of the photocatalysts was further analyzed by N2 adsorption–desorption experiment (Fig. 5). The calculated specific surface areas of BiVO4, BC, BBC-1, BBC-2, BBC-3, and BBC-4 were 6.48, 7.11, 12.33, 20.48, 28.09, and 21.76 m2 g−1, respectively. The SEM images show that the catalyst surface is covered with small nanoscale pores (10–20 nm) and other slit-type pore channels are formed due to the accumulation of agglomerates on each other. Generally, when the specific surface area of the material is large, plenty of pollutant molecules are easily absorbed by the material. The rapid contact between pollutants and photogenerated strong oxidizing substances speeds the photocatalytic progress.33,34
The light absorption band gap variation was analyzed by DRS. All catalysts have good absorption of the visible light (Fig. 6a). The absorption wavelengths of the composite catalysts all lie between the BiVO4 (510 nm) and CdS (584 nm) (Table S1†).
Fig. 6 (a) UV-vis DRS of the prepared catalysts and (b) the corresponding (αhν)2 vs. hν plots. Valence-band XPS spectrum of BiVO4 (c) and CdS (d). |
At the same time, all the composite catalysts produce different degrees of redshift compared with that of BiVO4, in which BBC-3 exhibited the largest absorption expansion. Because of the interfacial interaction between BiVO4 and CdS, the absorbing light range of the catalyst expands. At the same time, BBC exhibits the porous structure of wood, and it can transmit sufficient light and obtain a large range of light absorption, which enhances the light responsiveness. Normally, the wider the optical absorption wavelength, the stronger the photoresponse. The forbidden bandgap of the semiconductor can be estimated by eqn (1) as follows:
(αhν)1/n = A(hν − Eg) | (1) |
Photocatalyst | Solution | Removal efficiency (adsorption equilibrium) | Reference |
---|---|---|---|
Balsa templated-BiVO4–CdS | 10 mg per L RhB | 29.26% | This work |
Hollow CdS/BiVO4 | 15 mg per L RhB | 0.536% | 38 |
BiVO4–CdS | 20 mg per L TCH | 1.435% | 14 |
SDBC–BiVO4–CdS | 20 mg per L TCH | 3.138% | 14 |
PVP–BiVO4–CdS | 20 mg per L TCH | 6.384% | 14 |
EDTA–BiVO4–CdS | 20 mg per L TCH | 9.221% | 14 |
BiVO4–Au@CdS | 5 mg per L RhB | 9.248% | 39 |
Hierarchical construction Bi/BiVO4–CdS | 20 mg per L TCH | 20.865% | 40 |
Then, the effects of different loading amounts of Pt on the H2 production and RhB degradation efficiency were investigated using BBC-3. As shown in Fig. 8b, the rate of H2 production and RhB degradation increased as the Pt loading increased from 0.5% to 1%, while the rate of H2 production and RhB removal decreased a little as the Pt loading increased from 1% to 2%. This situation occurs because Pt clusters form on the surface of BBC-3 when the loading amount of Pt exceeds 1%, which reduces the availability of this part of Pt; as a result, the efficiency of photogenerated electron–hole separation decreases and the photocatalytic ability of the catalyst weakens.41,42
In addition, the effect of the initial concentration of RhB solution on the photocatalytic H2 generation of BBC-3 was further studied. As the initial concentration of RhB solution increased, the rate of H2 generation increased first and then decreased. The fastest rate of H2 production was achieved at an initial RhB concentration of 10 mg L−1 (Fig. S2a†). When the dye concentration initially increases, more RhB molecules adsorb to the catalyst surface, which in turn can interact with the photogenerated electron holes more rapidly. As the RhB concentration further increases, the irradiation of some visible light through the water bodies to BBC-3 is hindered, leading to a lower rate of H2 production.43 Finally, the long-term stability of BBC-3 was examined by four rounds of cycling experiments (Fig. 8d). After four consecutive cycles (Fig. S2b†), the rate of H2 generation decreased slightly (61.2 → 57.31 μmol g−1 h−1), and the rate of synergistic degradation of RhB remained almost unchanged (98.33 → 95.27%). The results indicate that BBC-3 exhibits excellent long-term stability and photocatalytic activity.
The photogenerated electron–hole complexation rate is a key factor that affects the photocatalytic performance of photocatalysts. The photogenerated electron–hole separation of the prepared catalysts was investigated by fluorescence spectra, photocurrent response, and EIS spectra. Fig. 9a shows the PL spectra of BiVO4, CdS, BC, and BBC-3. Compared with BiVO4 and CdS, both BC and BBC-3 exhibit a significantly weaker fluorescence intensity, and the fluorescence intensity of BBC-3 is the weakest, indicating that photogenerated electron–hole complexation is inhibited in the presence of heterojunctions, and the electron–hole on BBC-3 exhibits the best separation efficiency.44 Photoelectrochemical experiments were then performed, the photocurrent response of BBC-3 is much higher than those of BiVO4, CdS, and BC (Fig. 9b), which indicates that photogenerated electron–holes are more readily transferred to the surface for redox reactions through the channels formed by the wood template, which is consistent with the photoluminescence results.45 EIS spectra were used to elucidate the migration of photoexcited electron–holes. In the Nyquist plot, the arc radius represents the equivalent resistance, and the larger the arc radius, the higher the recombination of the photoexcited electron–hole.46 The semicircular radius of BBC-3 is smaller than those of BiVO4, CdS, and BC (Fig. 9c), thus indicating that BBC-3 shows a higher migration efficiency for photogenerated carriers.
To clarify the principle of synergistic H2 production from RhB photodegradation, trapping experiments were performed to investigate the main active species in the photocatalytic process on BBC-3. Hydroxyl radical (·OH) and hole (h+) trapping experiments were performed by adding t-Bu(OH)2 and EDTA-2Na, respectively. When adding t-Bu(OH)2 to the system, the degradation rate of RhB was somewhat affected, and it was hardly affected by the efficiency of H2 production. When EDTA-2Na was present in the system, the rate of H2 production and the removal rate of RhB decreased greatly. The results of the active species trapping indicated that both h+ and ·OH were involved in the RhB degradation process, while ·OH was basically not involved in the photocatalytic H2 production process, and h+ is the main active substances for photocatalytic degradation and photocatalytic H2 production. These results further demonstrate that RhB acts as a sacrificial electron donor and scavenges photogenerated holes to promote H2 production while leading to its own decomposition (Fig. S2c†).
The results of photodegradation of RhB with simultaneous production of H2 illustrated that the complexation of CdS improved the photoresponsiveness of BiVO4 and that the replication of wood micromorphology exhibited a better adsorption ability. To elucidate the photocatalytic mechanism of this system, the empirical equation Eg = EVB − ECB was used to calculate the conduction band (CB) potentials of pure BiVO4 and CdS.47 According to the calculated EVB of BiVO4 and CdS, it is calculated that ECB-BiVO4 = 0.15 eV and ECB-CdS = −0.78 eV (vs. NHE). Apparently, when BiVO4 and CdS are hybridized, suitable band structures can be established to improve the electron–hole pair efficiency.
In addition, the RhB molecules adsorbed on the catalyst surface can generate electrons by photoexcitation, and the LUMO and HOMO of RhB are −1.42 and 0.95 eV, respectively.48,49 Since the LUMO site of RhB is more negative than the CB of BiVO4 and CdS, photogenerated electrons can be delivered to BiVO4 and CdS. In this way, the large amount of foreign electrons that are injected increases the carrier migration rate between the catalyst interfaces, which in turn enhances the photocatalytic efficiency. The carrier transfer mode is discussed below.
If the electron transfer between BiVO4 and CdS follows the traditional type II heterojunction, then the photogenerated electrons will transfer from the CB of CdS to the CB of BiVO4, and the photogenerated holes will transfer from the VB of BiVO4 to CdS. At this time, the electrons and holes will accumulate at the CB of BiVO4 and the VB of CdS, respectively. Since the reduction potential of H2 is more negative than the CB of BiVO4, and the oxidation potential of ·OH is more positive than the VB of CdS, then H2 and ·OH cannot be produced, which is inconsistent with the experimental results. Therefore, the transfer of carriers should follow a more reasonable mechanism, the Z-scheme transfer mechanism.
The irregular BiVO4–CdS agglomerates improve the transfer efficiency of photocatalytic products and RhB molecules at the interface due to the three-dimensional pore structure of wood.50,51 The BBC rapidly adsorbs a large number of RhB molecules, and subsequently, the RhB molecules are excited by light and generate electrons that are inputted onto the CB of BiVO4 and CdS. In the heterojunction of BiVO4–CdS, the electrons in the CB of BiVO4 can be rapidly moved to the VB of CdS to regroup with the photogenerated holes it produces. At this point, the photogenerated holes of BiVO4 and the photogenerated electrons of CdS are retained. The holes in the VB of BiVO4 and the electrons in the CB of CdS produce ·OH and H2 during photoexcitation, which is consistent with the photocatalytic results (Fig. 10). RhB was removed by its own supply of electrons while being oxidized by ·OH. Through this photogenerated carrier transfer mode, the composite BiVO4–CdS exhibits better redox performance to degrade pollutants while generating hydrogen, making BBC-3 a good dual-functional catalyst.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2ra06735h |
This journal is © The Royal Society of Chemistry 2023 |