Open Access Article
Rundong Maab,
Yihui Sun
c,
Hui Zhangc,
Jie Zhuc,
Han Tiana,
Xiong Guoc,
Ruifen Wangc,
Xiangzhi Cui
*a,
Xinmei Hou
b and
Shengli Anc
aShanghai institute of Ceramics, Chinese Academy of Sciences, Shanghai, China. E-mail: cuixz@mail.sic.ac.cn
bBeijing University of Science and Technology, Carbon Neutrality Institute, Beijing, China
cSchool of Materials and Metallurgy Inner Mongolia University of Science and Technology, Baotou, China
First published on 19th June 2024
In recent decades, environmental protection and energy issues have gained significant attention, and the development of efficient, environmentally friendly catalysts has become especially crucial for the advancement of photocatalytic technology. This study employs the sintering method to produce biochar. A hybrid photocatalyst for the degradation of RHB under visible light was prepared by loading varying proportions of biochar onto g-C3N4 using ultrasonic technology. Among them, 2% CGCD (2% biochar/g-C3N4) achieved a degradation rate of 91.3% for RHB after 30 minutes of visible light exposure, which was more than 25% higher than GCD (g-C3N4), and exhibited a higher photocurrent intensity and lower impedance value. The enhancement in photocatalytic activity is primarily attributed to the increased utilization efficiency of visible light and the electron transfer channel effect from a minor amount of biochar, effectively reducing the recombination of photo-generated charge carriers on the g-C3N4 surface, thereby significantly improving photocatalytic activity. The degradation of RHB is synergistically mediated by O2−, h+ (photo-generated holes), and ˙OH. The free radical capture experiment indicates that O2− and ˙OH are the primary active components, followed by h+.
Graphite phase carbon nitride (g-C3N4) is an excellent N-type semiconductor with stable physical and chemical properties, high surface charge density, which makes it easier to modify and regulate.4 Its two-dimensional layered structure similar to graphene gives it a large specific surface area, which also lays a good advantage in the field of photocatalysis.5,6 However, g-C3N4 suffers from poor visible light absorption ability, large bandgap width, and high recombination rate of photo generated charge carriers, greatly limiting its effective application in the field of photocatalysis.7,8 At present, many researchers have carried out a series of modification works on g-C3N4,9–11 such as microstructure control, heterojunction loading/construction, element doping, etc.12,13 Dai et al. prepared g-C3N4/Ag3VO4 composite materials containing Ag nanoparticles using chemical deposition method, and tested the photocatalytic degradation effect of MB under visible light. The results showed that the optimal photocatalytic performance was achieved when the ratio of Ag3VO4 to g-C3N4 was 5
:
2. The improvement of photocatalytic performance of composite materials is due to the strong coupling heterojunction formed between Ag3VO4 and g-C3N4. In addition, the porous structure of g-C3N4 and the surface plasmon resonance (SPR) effect of Ag accelerate the separation and transport of photo induced electron hole pairs, and effectively reduce carrier recombination.14 The composite modification of noble metal nanoparticles and ion doping can effectively reduce the recombination rate of g-C3N4 carrier and greatly improve photocatalytic efficiency. However, the preparation of this type of composite catalyst typically requires electrochemical deposition and hydrothermal methods, which may increase the cost of catalyst preparation and reduce the yield of the catalyst. Meanwhile, charge transfer at heterogeneous interfaces is often considered an important reason for the improvement of catalyst activity, and there is currently limited progress in this research.
Owing to the low loading/doping costs, as well as their ease of scaling up and industrialization.15 Carbon-based functional materials are playing a vital role in environmental protection, electrochemistry, and photocatalysis,16 with vast research opportunities ahead.
Biochar is the product of high-temperature pyrolysis of biomass under anaerobic conditions. Due to its low cost, environmental friendliness, and ease of preparation, biochar has also been widely used in various research fields, such as catalysis and the adsorption of heavy metal ions in soil.17,18 The graphite structure in biochar also endows it with good photoelectric properties. Luo et al. prepared tea residue biochar/g-C3N4 composite photocatalyst using high-temperature calcination method for reducing uranium in water.19 The results show that the removal rate of U(VI) by the composite photocatalyst TBC/g-C3N4 composite material can reach 99.64%, which is much higher than that of pure g-C3N4 (58.8%). The photogenerated electrons on the conduction band of g-C3N4 transitioning to TBC can effectively delay the recombination of g-C3N4 photogenerated carriers.20 Wang et al. prepared magnetism γ−. The catalytic performance of Fe2O3/O2-g-C3N4/BC composite material was tested. The results showed that the composite photocatalyst can rapidly and completely degrade the antibiotic sulfamethoxazole (SMX), with a mineralization rate of up to 62.3%. Sulfates and hydroxyl radicals are the main species in photocatalytic reactions.21
In this article, we prepared biochar using calcination method under anaerobic conditions, and prepared biochar/g-C3N4 (x% CGCD, x = 1, 2, 3, 5) composite catalyst with easy amplification and simple operation using ultrasonic composite method. Then, we characterized the microstructure of the prepared catalyst, tested its photoelectrochemical properties, and applied the catalyst to the degradation of RHB. The characteristics and advantages of composite catalysts were comprehensively analyzed from the perspectives of charge transfer, utilization of light and bandgap transformation, as well as the degradation mechanism of RhB.
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100, respectively. The particles were dispersed in 30 mL of ethanol and 40 mL of deionized water using ultrasound for 2 hours, then stirred with a magnetic stirrer for 2 hours to obtain a biochar/g-C3N4 composite photocatalyst, denoted as X% CGCD (X = 1, 2, 3, 5).
| η = (A0 − A)/A0 × 100% = (C0 − C)/C0 × 100% | (1) |
In the eqn (1), η represents the photocatalytic degradation efficiency, A0 represents the initial absorbance of RHB, A represents the absorbance at the time of sample removal, C0 is the initial concentration, C is the concentration value of RHB at different time periods. Typically, A value is the absorbance of RHB at 554 nm, which is the maximum absorbance of RHB solution. This is also used to distinguish RHB from other organic compounds. The photocatalytic performance of the sample was tested using the Beijing Perfect light PCX-50C multi-channel photochemical reactor, with a light intensity of 260 mW cm−2.
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| Fig. 2 XRD spectra of different samples. (a) XRD comparison of wheat straw biochar before and after acid leaching; (b) XRD patterns of different samples. | ||
Fig. 3 shows the SEM and HR-TEM images of different samples. Wherein, Fig. 3a shows the powdered biochar obtained by direct grinding after calcination and preparation, which presents an irregular block shape; Fig. 3b shows the biochar washed via HCL, and its surface exposes a rich microporous structure, which indicates that the corrosion of hydrochloric acid can effectively increase the specific surface area of biochar. Fig. 3c shows the microscopic morphology of g-C3N4 (GCD). The results indicate that the sample exhibits a block/layered structure formed via the stacking of nanosheets, which is formed via the gradual stacking and recombination of g-C3N4 molecules. Fig. 3d shows the microstructure of 2% CGCD, which can be seen to be formed via the continuous stacking of nanoparticles or nanosheets of varying sizes. Fig. 3e and f shows the HR-TEM images of 2% CGCD, and it can be observed that the sample after ultrasonic treatment still maintains a nanosheet morphology. In Fig. 3f, lattice stripes on the (002) crystal plane of g-C3N4 in the composite sample can be observed, with a crystal plane spacing of 0.33 nm. This also proves the good mechanical stability of g-C3N4, which is consistent with the analysis of XRD results.
The functional groups of the sample were characterized using FT-IR spectroscopy. As depicted in Fig. 4a, the reflection peak at 2820 cm−1 is attributed to the stretching vibration of the relevant N–H bonds, which belong to the non-condensed NH2 groups.24,25 The reflection peak at 3500 cm−1 is due to the vibration (surface adsorption) of hydroxyl (−OH) in the associated state,26 likely resulting from the adsorbed oxygen formed by the sample's interaction with ethanol and water molecules during ultrasonic treatment. This peak range is absent in the biochar's spectral profile, likely attributed to the binding of H+ with surface hydroxyl groups during the acid leaching process, or it may be related to the size of biochar pores. As shown in Fig. 4b, it is observed that as the biochar dosage increases, the intensity of the absorption peak at 1600 cm−1 of the heptane triazole ring varies, signifying that the introduction of biochar alters the chemical environment surrounding g-C3N4, indicating successful composite formation between the two samples.
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| Fig. 4 FT-IR spectra of different samples; (a) FT-IR diagrams of different samples before and after recombination; (b) FT-IR spectra of composite photocatalysts. | ||
The surface elemental composition of GCD and 2% CGCD was analysed by using XPS. Fig. 5a displays the total spectrum of the photocatalyst, revealing three elements, C, N, and O, in the XPS spectrum. Notably, 2% CGCD has a larger O peak area, indicating an increase in oxygen atoms adsorbed on the surface of the composite sample. Fig. 5b shows the spectral peak of the C 1s energy level in the sample. Among them, the binding energy at 287.6 eV corresponds to the N–C
N characteristic peak of sp2 hybrid C in GCD, the peak at 398.2 eV in Fig. 5c corresponds to the C
N–C structure in GCD,27 and the peak at 399.75 eV corresponds to the –NH2 group of non-polymerizations, which together form triazine ring structural units. From Fig. 5b and c, it can be seen that in the composite sample, all three peaks shift towards higher chemical shifts, indicating the presence of charge transfer on the surface of the triazine ring, which mainly shows a trend of losing electrons. This indicates that biochar, as a charge transfer channel, can attract electrons from the conduction band of GCD, and the two exhibit strong interactions. As shown in Fig. 5d, the positions at 530.35 eV, 532.6 eV, and 533.8 eV correspond to the C
O, C–O, and O–C (O) bonds, respectively. Among them, the C
O content in 2% CGCD is significantly lower than that in GCD, and the binding energy undergoes a red shift, indicating that ultrasound method has a destructive effect on the C
O bond, which is more conducive to the recombination of BC and GCD.28
N2 adsorption desorption and pore size distribution tests were conducted on different samples. As shown in Fig. 6a–c, the pore types of powdered GCD are mostly mesoporous structures, with a pore size of approximately 48 nm; The pore size of 2% CGCD is approximately 40–50 nm, slightly larger than that of GCD. This can be attributed to the fragmentation and formation of smaller particles and nanosheets in bulk GCD under ultrasound action. BC has abundant micropores and a small amount of mesoporous structure. Among them, the pore size of the micropores is about 3–4 nm, which may be attributed to the pores left by the evaporation of water molecules during the combustion of lignin and cellulose in wheat. The mesoporous pore size is approximately 30–40 nm, which may be attributed to the collapse and merging of micropores. All three samples have hysteresis loops, and the shape of the pores is mostly H4-type fine pores formed by the stacking of layered molecules, which is consistent with the characterization results of SEM and XRD. Table 1 shows the statistical distribution of sample specific surface area. It can be observed that the specific surface area of GCD located between biochar and GCD is about 73.9 m2 g−1, and the specific surface area of the composite photocatalyst sample is about 66.7 m2 g−1. This may be related to the shortening of the spacing between GCD crystal planes in the composite sample, indicating the successful recombination of the two samples.29
| Sample name | GCD | BC | 2% CGCD |
|---|---|---|---|
| BET surface area (m2 g−1) | 73.87 | 7.10 | 66.73 |
As shown in Fig. 6d, the absorption edge of pure graphite phase carbon nitride is about 455 nm. As the amount of biochar introduced increases, the absorption band edge gradually shifts to red, indicating a significant improvement in the response of the photocatalyst to visible light. As shown in Fig. 6e, according to the formula Eg = 1240/λ, the estimated bandgap of g-C3N4 is approximately 2.72 eV. Meanwhile, according to the Tauc plot formula, a Tauc plot is drawn, which also satisfies this condition, the Tauc plot also satisfies this condition The position of the valence band (VB) and conduction band (CB) of GCD can be calculated according to formulas (2) and (3). In the formula, Ec is the dipole moment of the standard hydrogen electrode, which is 4.5 eV in value, Eg is the band gap width of the semiconductor, and ECB and EVB represent the conduction band and valence band values of the semiconductor, respectively. X is the absolute electronegativity of the semiconductor, which is numerically equal to the geometric average value of each component atom in the semiconductor. Through consulting the literature, the empirical value of XGCD is 4.73,30 and further calculation shows that its EVB and ECB are 1.13 eV and −1.59 eV, respectively. In order to further refine the band data, we conducted XPS valence band spectrum testing, the top energy of GCD's CB is 1.17 eV, which is close to the calculated value (Fig. 6d). With the increase in biochar, the band gap of the composite photocatalyst is shorter than that of pure g-C3N4, and the absorption band edge is gradually red shifted, indicating that the introduction of biochar enhances the response of the g-C3N4 system to visible light, and shortens its band gap, which is more conducive to the transition of photogenerated carriers and increases the charge density of the catalyst surface, thus improving the activity of the photocatalyst.
| ECB = X − EC − Eg/2 | (2) |
| EVB = ECB + Eg | (3) |
The recombination of photo-generated carriers in the sample was analysed via PL fluorescence spectroscopy. As shown in Fig. 6f, when visible light's energy is greater than the sample bandgap used to irradiate the sample, the photo-generated electrons undergo energy level transitions. When photo-generated charge carriers recombine, some of the energy is released in the form of phonons, manifested as lattice vibrations, while the other part is released in the form of photons (fluorescence).31 From the figure, it can be seen that with an excitation of 370 nm wavelength light, the carrier recombination rate of 2% CGCD is significantly lower than that of pure graphite phase carbon nitride. Biochar does not produce fluorescence in this band, indicating that the introduction of biochar significantly reduces the recombination of g-C3N4 carriers, which helps to efficiently carry out photocatalytic reactions.
| ln(C0/C) = kt + constant | (4) |
| Sample name | GCD | BC | 1% CGCD | 2% CGCD | 3% CGCD | 5% CGCD |
|---|---|---|---|---|---|---|
| Rate constant (k/min−1) | 2.53 × 10−2 | 0.9 × 10−2 | 3.29 × 10−2 | 3.88 × 10−2 | 3.63 × 10−2 | 3.09 × 10−2 |
| R2 | 0.929 | 0.877 | 0.914 | 0.908 | 0.925 | 0.924 |
Fig. 7d shows the cyclic performance test of 2% CGCD. After five cycles of experiments, the degradation rate of RHB in the sample can still reach 91.7%, indicating that the sample has good photocatalytic stability. The 2% CGCD sample after cycling was characterized via secondary XRD, as shown in Fig. 7e. After 5-times' cycling, the (100) and (002) crystal plane diffraction peaks of g-C3N4 in the sample did not show a red or blue shift, indicating that the sample can still maintain its stable phase structure after cycling testing. After cyclic testing, the diffraction peaks of the composite photocatalyst on the (100) and (002) crystal planes slightly decreased, which may be due to the slight damage and de-formation of the crystal state of the catalyst sample caused via ultrasound and washing. With tert-butyl alcohol, KI, and BQ as quenching agents, the photocatalytic degradation experiments of ˙ OH, h+, and O2− were carried out, respectively. As shown in Fig. 7f, after the addition of tert-butyl alcohol, potassium iodide, and p-benzoquinone, the degradation rates of RHB via the composite photocatalyst de-creased to 46.15%, 75.42%, and 41.2%, respectively. It can be concluded that the main active species in the photocatalytic degradation experiment are ˙ OH and O2−, followed by h+. Due to the negative conduction band potential of GCD, it is more conducive to the reduction reaction of surface-adsorbed O2 and the generation of active species such as O2− and ˙ OH. At the same time, GCD belongs to N-type semiconductors, and its surface has a high e− density, while the density of h+ is relatively small, which may also make its oxidation effect less obvious.36,37
To delve into the separation and recombination of charge carriers in biochar/g-C3N4 composite samples, transient chronoamperometry and electrochemical impedance spectroscopy were applied to the catalyst before and after the recombination process. As depicted in Fig. 8a, the transient current intensity of 2% CGCD is notably greater than that of GCD, implying that the composite photocatalyst boasts an outstanding level of photo-induced carrier separation, thereby facilitating carrier migration at the membrane electrode/electrolyte interface. The arc radius on the EIS spectrum is linked to the charge transfer at the interface between the working electrode and electrolyte,38 as illustrated in Fig. 8b. The arc radius of the EIS electrode reflects the charge transfer resistance in the electrode/electrolyte solution, with a larger radius corresponding to a higher charge transfer resistance. Notably, the charge transfer resistance of 2% CGCD is significantly reduced compared to that of pure graphite phase carbon nitride, indicating that the composite sample exhibits reduced electrode/electrolyte transfer resistance and enhanced charge transfer capability.
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| Fig. 8 Electrochemical characterization of different samples; (a) electrochemical characterization test of composite photocatalysts; (b) electrochemical AC impedance spectroscopy. | ||
C structure, ultimately mineralizing RHB into H2O and CO2.39 The second type is the reduction reaction between the reducing electrons transitioning to the conduction band in photocatalysts and the catalyst surface in solution, yielding O2− with strong redox properties. Owing to the unpaired electrons in O2−, it also exhibits strong redox characteristics and can mineralize and degrade RHB. In the third pathway, because of the N-type semiconductor properties of GCD, photo-generated electrons originate not only from the 2p orbital of C in GCD but also from the 2p orbital of N. As a result, the reduction reaction on the GCD surface is quite active, likely generating an excessive amount of O2−. O2− can also react with H+ in water, producing a strong oxidizing and non-selective hydroxyl radical (˙OH), thereby oxidizing and degrading RHB. During the degradation process of RHB, photogenerated holes, O2−, and ˙OH exhibit a synergistic effect.
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