Abstract
Highly active Ti/Sb–SnO2 electrodes were fabricated using sol-gel spin coating procedure, which exhibited a rough, uniform and multilayer coating structure. The effects of different Sb-SnO2 film layers on the physiochemical, electrochemical properties and pollutant degradability of electrodes and the mechanism were evaluated on a systematic basis. The electrodes with more active layers exhibited higher electro-catalytic performance. Upon exceeding 8 layers, the promotion effect of the coating was reduced. Considering various factors, this paper recommends preparing Ti/Sb–SnO2 electrodes coated with 8 layers to obtain higher electro-catalytic ability in landfill leachate treatment. The specific number of coating layers should be determined according to the electrode requirements. This work provided a theoretical basis and technical support for the preparation of Ti-SnO2 electrodes with high electro-catalytic activity and stability, while it still remains a great challenge to achieve an excellent balance between performance and stability before Ti/Sb-SnO2 electrodes can be implemented on a large scale in wastewater treatment.
HIGHLIGHTS
Sol-gel spin coating method could be used to exhibit a multilayer coating structure.
Electrodes with more active layers had higher electro-catalytic performance.
Upon exceeding 8 layers, the promotion effect of the coating was reduced.
Ti/Sb-SnO2 electrodes coated with 8 layers could obtain higher electro-catalytic ability during leachate treatment.
Graphical Abstract
INTRODUCTION
In recent years, nearly 80% of the world's population is threatened by water security on a global scale (Vörösmarty et al. 2010). One of the most important reasons for water pollution is the massive discharge of refractory organic wastewater (Han et al. 2018), which is characterized by high organic load, complex characteristics and strong bio-inhibition (Sun et al. 2019). The most representative one is landfill leachate, which contains a large amount of pollutants such as biodegradable and refractory organics, inorganic salts (e.g., Na+, NH4+) and heavy metals (Zhang et al. 2020a, 2020b). The generation of leachate is anticipated to increase as the amount of landfilled solid waste continues to grow globally (Feng et al. 2021). Electrochemical Advanced Oxidation Processes (EAOPs) emerge as a promising technology in the field of organic wastewater treatment (Seibert et al. 2020). Compared to traditional biological treatment methods, EAOPs has shown greater advantages like high efficiency, no requirement for chemicals and low-volume application (Ganiyu et al. 2018).
Nowadays, three kinds of electrodes, namely tin dioxide (SnO2) (Mora-Gomez et al. 2019), lead dioxide (PbO2) (Tan et al. 2011) and boron-doped diamond (BDD) (Olvera-Vargas et al. 2021) have attracted great attention from researchers because of high oxygen evolution potentials (OEP), which could favor the large production of reactive oxygen species to destroy organic matters (Skoumal et al. 2008; Moradi et al. 2020). BDD has proven to be the most potential material for anodic oxidation of organics (Olvera-Vargas et al. 2021). However, the high cost of BDD restricts its widespread commercial applications (Brillas et al. 2005; Ciríaco et al. 2009). PbO2 electrode has shown excellent catalytic performance, long service lifetime and low cost as a non-active anode, but it also has some shortcomings such as secondary contamination due to Pb dissolution (Yao et al. 2019; Li et al. 2020a, 2020b, 2020c). Generally speaking, SnO2 cannot be directly used as an electrode coating material due to high resistance (Mora-Gomez et al. 2019). A number of researchers focused on the enhancement of OEP, service lifetime and current efficiency of SnO2 electrodes (Chen et al. 2018). Doping is a powerful approach for modulating the electrical properties of metal oxides (Malviya et al. 2017). It was reported that Sb doped SnO2 coating could not only greatly improve the conductivity of electrodes, but also led to higher electrochemical stability (Chen et al. 2020).
There are four main methods that can help to prepare antimony-doped tin oxide (Ti/Sb–SnO2): dip-coating (Zhou et al. 2019), electrolytic deposition (Sun et al. 2020a, 2020b, 2020c), spin coating (Sivakumar et al. 2021) and pyrolysis spray (Elangovan et al. 2005). Based on the above-mentioned preparation method, Ti/Sb–SnO2 electrodes have been widely used in various kinds of wastewater treatment (Maharana et al. 2015; Zhang et al. 2020a, 2020b). Researchers usually used co-doped SnO2-Sb–x (x-element) (Endoh & Kurihara 1998; Duan et al. 2014), interlayer insertion (Li et al. 2020a, 2020b, 2020c) and Ti substrate modification (Hodges et al. 2018) to further enhance the service life and electro-catalytic property of Ti/Sb–SnO2 electrode (Aguilar et al. 2018).
Most of the previous studies have focused on the parameter adjustment of electrode preparation such as solvent type (Sun et al. 2020a, 2020b, 2020c), metal element ratio (Elangovan et al. 2005) etc, while a few were devoted to the effects of different Sb-SnO2 coating layers and practical application of landfill leachate treatment. The objectives of this paper were to: (1) to provide a sol-gel spin coating method to fabricate Ti/Sb–SnO2 electrodes that could exhibit a rough, uniform and multilayer coating structure; (2) to systematically assess the effects of different Sb-SnO2 film layers on physiochemical, electrochemical properties and pollutant degradability of Ti/Sb–SnO2 electrodes; and (3) to reveal the mechanism of electrochemical activity of electrodes with different coating layers, further providing theoretical guidance and technical support to prepare the electrodes with high electro-catalytic activity and stability in the field of wastewater treatment.
METHODOLOGY
Electrode preparation
A four-step procedure involving titanium substrate pretreatment, precursor reagent preparation, sol-gel spin coating and subsequent calcination process was used to form an Sb-SnO2 coating on Ti substrates to prepare Ti/Sb-SnO2 electrodes (Figure 1) (Comninellis & Vercesi 1991). Ti substrates (3 cm × 3 cm × 1 mm) were initially polished by 100-grits, 500-grits and 1000-grits sandpapers and then successively washed with acetone and deionized water. Then, clean Ti plates were soaked in 35 wt% oxalic acid solution, which was heated at 100 °C for 2 h until TiO2 was thoroughly dissolved. The resulting Ti substrates were preserved in acetone for further use (Jin et al. 2020).
The Sb-SnO2 coating was prepared on Ti substrates by employing the sol-gel spin coating method. For the preparation of precursor reagent, a mixture of SnCl4 5H2O and SbCl3 at molar ratio of 10:1 was dissolved in water at a low pH. When completely dissolved, a certain amount of citric acid was added and polyethylene glycol was also added into the solution. After ultrasonic treatment, agitation and aging treatments, the resulting reagent was sealed for further use. The reagent was spin-coated on the cleaned Ti substrates at the speed of 1,000 rpm for 10 s and 3,000 rpm for 15 s, followed by an evaporation treatment at 120 °C for 10 min and a calcination process at 500 °C for 10 min. The procedures (spin coating, drying, and sintering) were repeated 2, 4, 8, 12, and 16 times, respectively, and finally, the electrodes were annealed in a muffle furnace at 500 °C for 2 h.
Physicochemical characterization
Scanning electron microscopy (SEM, SU8010, Japan), X-ray diffraction (XRD, Bruker D8 Advance, Germany) study and X-ray photoelectron spectroscopy (XPS, Thermo Scientific K-Alpha + , USA) techniques were applied to characterize the surface morphology of Ti/Sb–SnO2 electrodes. The XPS data were corrected with reference to the C 1s peak at 284.8 eV.
Electrochemical characterization
The electrochemical characterization involved techniques like linear scanning voltammetry (LSV), cyclic voltammetry (CV) and tafel tests performed in 0.5 M H2SO4 solution on an electrochemical workstation (CHI1100C, Shanghai) with a platinum plate and saturated calomel electrode (SCE) as counter and reference electrode, respectively. LSV tests were run in the range of 0–3 V at a scan rate of 50 mV s−1. CV tests were performed over the voltage range of −1.0 to 0 V versus SCE at scan rate of 50 mV s−1. Tafel curves were obtained at 50 mV/s to explore the kinetics of oxygen evolution reaction.
Pollutant degradation experiment
The pollutant degradation tests were conducted in a stirred cell containing 100 mL landfill leachate (3,938.75 mg/L COD, 279.45 mg/L TN, EC = 11.92 mS/cm) that included 3,078 mg/L Cl− as a supporting electrolyte at room temperature. The basic physical-chemical characterization of the effluent is represented in Table 1. All the tests were carried out with the applied voltage of 4 V over a reaction time of 120 min. The prepared electrode was used as anode and titanium plate was used as cathode with a distance of 1 cm. Chemical oxygen demand (COD) analyses were carried out by rapid digestion spectrophotometric method with potassium dichromate using a benchtop VIS spectrophotometer (DR3900, Hach Company, USA). Total nitrogen (TN) analyses were conducted by Alkaline potassium persulfate digestion-UV spectrophotometric method. LSV tests were run before and after the electrode degradation.
COD (mg/L) . | TN (mg/L) . | TP (mg/L) . | NH3-N (mg/L) . |
---|---|---|---|
3,938.75 ± 2.75 | 279.45 ± 2.92 | 38.08 ± 0.95 | 152.03 ± 0.95 |
NO3−-N (mg/L) | pH | EC (mS/cm) | Cl− (mg/L) |
20.10 ± 0.07 | 4.74 ± 0.01 | 11.92 ± 0.23 | 3,078 ± 4.92 |
COD (mg/L) . | TN (mg/L) . | TP (mg/L) . | NH3-N (mg/L) . |
---|---|---|---|
3,938.75 ± 2.75 | 279.45 ± 2.92 | 38.08 ± 0.95 | 152.03 ± 0.95 |
NO3−-N (mg/L) | pH | EC (mS/cm) | Cl− (mg/L) |
20.10 ± 0.07 | 4.74 ± 0.01 | 11.92 ± 0.23 | 3,078 ± 4.92 |
RESULTS AND DISCUSSION
Physicochemical characterization
More detailed information on morphology can be obtained from the SEM images taken about the different coating layers of electrodes. Images having magnification of 1.0 K and 5.0 K are illustrated in Figure 2. The surface of the pre-treated Ti substrate presented a honeycomb structure having many cracks and holes (Figure 2(a)). After coating with Sb-SnO2 precursor solution, the electrodes presented a smooth and compact surface with fewer cracks on the catalyst layer, proving that a uniform oxide layer in firm contact with the Ti substrate had formed (Huang et al. 2020). An obvious porous structure was observed due to the evaporation of solvent during the heating process (Xiao et al. 2020). The electrode surface became denser and more compact as the layers increased within 8 layers, and the number of holes decreased, which was beneficial to increase the specific surface area and to enhance the bonding ability between the substrate and the coated layer. However, the electrodes coated with 12 and 16 layers presented a flat surface, indicating lower conductivity. The cracks on the surface of 16-coated electrodes increased compared with 12-coated electrodes. The phenomenon of crack production was attributable to the differences in the shrinkage or expansion properties between the Sn-Sb active layer and titanium substrate during calcination and the evaporation of solvent in the dry rubbing process (Bi et al. 2019a). The penetration of electrolyte into the substrate through these cracks would reduce the binding force between the coating and the substrate, which would seriously affect the electrochemical activity and stability (Li et al. 2020a, 2020b, 2020c).
To better elucidate the catalytic mechanism, the crystal structure of coating was analyzed by XRD pattern (Figure 3). The peak XRD positions of electrodes with different coating layers were basically similar, which were consistent with the data of JCPDS card 44-1294 on titanium matrix. Ti had a higher diffraction peak intensity due to X-ray penetration through the oxide coating during the test. The diffraction peaks of SnO2 were observed at 53.143°, 63.298°(JCPDS card 50-1429) and 26.495°, 33.727° (JCPDS card 46-1088). Doping of Sb ions in SnO2 coating could not be clearly discerned through the XRD spectrum (Yang et al. 2017), the reasons might be: 1. The Sb content was too low to be detected by XRD; 2. The element Sb might have entered into the lattice of SnO2 crystal by substitution. The diffraction peak width was inversely proportional to the grain size. The wider the peak width, the smaller the grain size. It could be deduced from the decreased grain size that the catalytic active sites of the electrode increased (Chen et al. 2018).
X-ray photoelectron spectroscopy (XPS) was performed to quantify O, Sn, and Sb on the electrodes, as well as to study their chemical states and stoichiometry. The core level 3d spectra of Sn are shown in Figure 4(a) and 4(b), the Sn 3d5/2 peak at 487 eV and the Sn 3d3/2 peak at 496 eV were observed for Ti/Sb-SnO2 electrodes, indicating a successful coating of SnO2 layer on Ti substrate (Wang et al. 2020), which was similar to the XPS peaks as reported by Choi et al. (1996). Due to low concentration, 3d Sb could not be clearly detected in the full spectrum, while the Sb 3d5/2 peak at 532 eV and the Sb 3d3/2 peak at 541 eV were observed in fine spectra, indicating that the antimony was bound with oxygen. As shown in Figure 4(c), the XPS peak of Sb 3d3/2 was weaker than Sb 3d5/2. The peak heights of Sn and Sb elements obviously increased with the increasing coating layers. The shift of peaks position to lower binding energy indicated a change in oxygen environment (Bjelajac et al. 2020). Sn 3d binding energies of 12 and 16 coating layers were lower than others, which might be owing to high average electron cloud density. Higher electron cloud density means less lattice oxygen and more oxygen vacancies, thus promoting the generation of hydroxyl radicals, which was basically consistent with the information reflected in the LSV curve. The O 1s spectrum of Sb–SnO2 coating was fitted by several peaks located at about 531 eV (Figure 4(d)), which was ascribed to lattice O (530 eV), surface adsorption oxygen (531 eV), and organic oxygen (533 eV), respectively (Kundu et al. 2008; Sun et al. 2020a, 2020b, 2020c). The peak in the figure is the result of the overlap of the above oxygen. As presented in Table 2, the oxygen peak tended to be 531 eV, indicating that the surface adsorption oxygen (Oads) was dominant while the lattice oxygen (Olat) was relatively fewer. Surface adsorption oxygen was directly related to the electrochemical oxidation process because it could participate in the direct oxidation or promote the generation of ·OH in the indirect oxidation. The Oads content of Ti/Sb–SnO2 electrodes coated with more layers was obviously larger, indicating stronger electro-catalytic ability was obtained.
Electrode layers . | Binding energy (eV) . | Oads content (%) Content = Oads/(Oads + Olat) × 100% . | |
---|---|---|---|
O1s (Olat) . | O1s (Oads) . | ||
2 | 530.13 | 531.61 | 95.78% |
4 | 530.18 | 531.96 | 97.03% |
8 | 530.33 | 531.83 | 96.61% |
12 | 530.98 | 532.02 | 96.57% |
16 | 530.16 | 531.33 | 99.19% |
Electrode layers . | Binding energy (eV) . | Oads content (%) Content = Oads/(Oads + Olat) × 100% . | |
---|---|---|---|
O1s (Olat) . | O1s (Oads) . | ||
2 | 530.13 | 531.61 | 95.78% |
4 | 530.18 | 531.96 | 97.03% |
8 | 530.33 | 531.83 | 96.61% |
12 | 530.98 | 532.02 | 96.57% |
16 | 530.16 | 531.33 | 99.19% |
Based on the above analyses, it was inferred that the substitution of Sn4+ by Sb5+ would increase the conductivities of the anodes due to excess electrons. Besides, permeating in Sn vacancies of SnO2, Sb as cationic doping could accelerate the charge transfer of the electronic conductor (Cobley et al. 2015).
Electrochemical characterization
The OEP value is a key parameter to evaluate the electro-catalytic ability of an electrode materials, and the higher OEP usually represents higher current efficiency for electrochemical degradation owing to fewer side reactions and lesser energy loss (Li et al. 2020a, 2020b, 2020c). As shown in Figure 5(a), the polarization curves of the electrodes were divided into two regions. The curve remained constant in the first region, while the current sharply increased in another region with increasing voltage. In the second region, a tangent was drawn where the curve abruptly arose, and the potential of the intersection of the tangent and the horizontal axis was the OEP of the electrode (Bi et al. 2019b). A comparison of the OEP of electrodes with different coating layers demonstrated the fact that the OEP slightly increased with the increasing coating layers (Figure 5(a)). The OEPs of electrodes coated with 8, 12 and 16 surface layers were around 1.8 V, while the 2 and 4 surface layers had 1.3 V and 1.4 V, respectively. Besides, the steady-state current under 2.1 V was basically linear with the coating layers. The main reasons could be: oxygen vacancies in the electrode surface had a great influence on OEP. SnO2, as an n-type semiconducting metal oxide, strongly depends on its non-stoichiometric composition (Feng et al. 2010). Higher electron cloud density could be obtained by applying more layers on the surface, which meant more oxygen vacancies were formed to promote the generation of hydroxyl radicals. While exceeding 8 layers, the effect of increasing the number of coating layers on improving OEP was not significant.
CV test was performed to measure the electro-catalytic activity of the electrodes. Generally, CV shows a series of anodic and cathodic peaks, representing the double-layer charging and the solid-state redox transition of the active oxides (Elgrishi et al. 2018; Liu et al. 2019). Voltametric charge (q*) was also measured to compare the number of active sites of the electrodes. q* is closely related to the conductive material, oxide content, surface morphology, dispersion, scanning speed, temperature and electrolyte, which was also an effective indicator of the dispersion degree of the catalyst in the coating (Wang et al. 2019). As presented in Figure 5(b), the degradation reaction of electrodes was mainly based on the quasi-reversible reaction. The voltametric charge (q*) initially increased and then decreased with increasing coating layers. The reason was that as the amount of effective substances in the metal oxide coated on the electrode surface kept increasing, the active coating layer was tightly and uniformly bound to the etched titanium matrix with good continuity; thereby, the electrode had a larger electrochemical active area (Voiry et al. 2018). Besides, the peak current density of the 8-active layer was higher under similar conditions in comparison to other electrodes, which showed that the electrodes with 8 active layers had a faster electron transfer rate (Bi et al. 2020). Electrodes with 12 and 16 active layers had higher OEP at the cost of conductivity. Therefore, the electro-catalytic performance of the electrode could be remarkably improved by coating the proper number of layers of the active substance.
Smaller was the slop of Tafel curve, the lower was the over-potential required to reach the specified current density, thus a higher electro-catalytic activity (Chen et al. 2018). As shown in Figure 5(c), there were obvious linear regions in each curve, which indicated that the oxygen evolution reaction was mainly controlled by electrochemical polarization (Mann & Thurgood 2011). As presented in Table 3, the Tafel slopes for the electrodes with 2, 4, 8, 12 and 16 coating layers were 0.208 dec−1,0.199 dec−1, 0.080 dec−1, 0.062 dec−1 and 0.057 dec−1 respectively. It could be deduced that electrodes with more coating layers possessed higher oxygen evolution activity, which accelerated the electrochemical transfer step. When exceeding 8 layers, the promotion effect of the coating was reduced.
Layers . | Ecorr(V vs.SCE) . | Cat Slp (V) . | Ano Slp (V) . | Cat Int (log i) . | Ano Int (log i) . |
---|---|---|---|---|---|
2 | 0.241 | 0.197 | 0.208 | −4.844 | −4.830 |
4 | 0.058 | 0.074 | 0.199 | −5.661 | −4.786 |
8 | −0.049 | 0.057 | 0.080 | −4.293 | −4.547 |
12 | −0.167 | 0.025 | 0.062 | −4.821 | −4.354 |
16 | −0.253 | 0.308 | 0.057 | −4.856 | −4.546 |
Layers . | Ecorr(V vs.SCE) . | Cat Slp (V) . | Ano Slp (V) . | Cat Int (log i) . | Ano Int (log i) . |
---|---|---|---|---|---|
2 | 0.241 | 0.197 | 0.208 | −4.844 | −4.830 |
4 | 0.058 | 0.074 | 0.199 | −5.661 | −4.786 |
8 | −0.049 | 0.057 | 0.080 | −4.293 | −4.547 |
12 | −0.167 | 0.025 | 0.062 | −4.821 | −4.354 |
16 | −0.253 | 0.308 | 0.057 | −4.856 | −4.546 |
As presented in Figure 5(d), the service life of the electrodes was calculated with 2, 4, 8, 12 and 16 coating layers, which were 0.5 min, 0.5 min, 10.3 min, 33.0 min and 58.7 min respectively. Obviously, the service span of the electrodes was proportional to the number of coating layers on the electrode surface. The industrial application of EAOPs is hindered by the short life service of Ti/Sb-SnO2 electrodes due to the low adhesion between the coating and the substrate (Sun et al. 2020a, 2020b, 2020c). In practical engineering application, the number of coating layers should be determined by considering both the service life and economic cost. It still remains a great challenge to achieve an excellent balance between performance, cost, and stability before Ti/Sb-SnO2 electrodes can be implemented on an industrial scale (Shao et al. 2017; Li et al. 2020a, 2020b, 2020c).
Pollutant degradation experiment
Shown in Figure 6 are the results of the removal efficiency of COD and TN with different Sn-Sb layers. Obviously, electrodes with 8 layers exhibited the highest COD removal efficiency (32.30%) and the highest TN removal efficiency (60.38%). As presented in Figure 7, although electrodes with 12 and 16 layers showed higher current densities before electrode invalidation, they had worse stability and lower current densities after electrode invalidation compared to the electrodes with 8 layers. With the increase of the number of coating layers, the increase of current density could be ascribed to the increased amount of active material, which enhanced the number of electro-excited carriers. However, once the Sb-SnO2 film thickness reached a certain threshold, charge carrier recombination became increasingly important, since the very short carrier diffusion length effectively limited the ability to remove charges from the electrode (Wang et al. 2011). Besides, electrodes with excess layers appeared to have larger particle size and lower coating adhesion that would also influence the electrode catalytic activity and pollutant degradation effect, which was consistent with the information reflected in the above electrochemical characterization. It was detected that Cl− concentration decreased from 3,078 mg/L to 1,998 mg/L before and after the electrolysis, indicating the formation of active chlorine species during the catalysis process. The organics degradation path, active species degradation mechanism, carbon and nitrogen balance were under way in our lab.
CONCLUSION
Ti/Sb–SnO2 electrodes with different active layers were fabricated using the sol-gel spin coating method. Various tests like LSV, CV, Tafel and ASL demonstrated that electrodes with more active layers had higher electro-catalytic performance, indicating a uniform, rough and highly active electrode surface was developed. When exceeding 8 layers, the promotion effect of the coating was reduced. Considering various factors, this paper recommends preparing Ti/Sb–SnO2 electrodes coated with 8 layers to get higher electro-catalytic ability and stability in wastewater treatment. The specific number of coating layers should be determined according to the electrode's requirements. It still remains a great challenge to achieve higher stability by increasing the binding energy before Ti/Sb-SnO2 electrodes could be implemented on full-scale in wastewater treatment.
ACKNOWLEDGEMENTS
This work was financially supported by the National Key Research and Development Program of China(Grant No. 2020YFD1100401).
DATA AVAILABILITY STATEMENT
All relevant data are included in the paper or its Supplementary Information.