Open Access Article
This Open Access Article is licensed under a Creative Commons Attribution-Non Commercial 3.0 Unported Licence

Sequencing batch photocatalytic H2O2 production over a magnetic resorcinol–formaldehyde polymer for on-site water purification by UV light irradiation

Jingzhen Zhang a, Qian Zheng a, Chen Chen b, Xiangcheng Zhang a, Xiaoyan Guo c and Mingce Long *a
aSchool of Environmental Science and Engineering, Key Laboratory of Thin Film and Microfabrication Technology, Ministry of Education, Shanghai Jiao Tong University, Shanghai 200240, China. E-mail: long_mc@sjtu.edu.cn
bShanghai Waterway Engineering Design and Consulting Co., Ltd, Shanghai 200120, China
cKey Laboratory of Pollution Processes and Environmental Criteria, College of Environmental Science and Engineering, Ministry of Education, Nankai University, Tianjin 300350, China

Received 25th September 2022 , Accepted 27th October 2022

First published on 28th October 2022


Abstract

A self-maintainable decentralized water treatment system is appealing, while avoiding chemical addition is the prerequisite to realize it. As a widely used chemical in advanced oxidation processes (AOPs), H2O2 can be produced via photocatalysis. However, there remain challenges to use the photocatalytically produced H2O2 for water purification in a continuous operation, which requires that the produced H2O2 solution has no impurity and the catalyst powder is easily separable. We realized this by photocatalytic H2O2 production over magnetic separable photocatalytic microspheres through a sequencing batch process and coupling with ultraviolet C (UVC)/H2O2 for micropollutant removal via a flow-through operation. The photocatalysts were synthesized by in situ growth of a resorcinol–formaldehyde (RF) copolymer on Fe3O4@SiO2 microspheres, which can convert earth-abundant water and air into H2O2 under visible light irradiation. A clean H2O2 solution was produced at 100 μmol h−1 g−1 over magnetic photocatalysts and separated by using an external magnetic field. The on-site utilization of the obtained H2O2 solution was realized via UV light irradiation. This work provides a rational design of easily separable photocatalysts for H2O2 production, and offers insights for development of water purification processes with zero chemical addition and maintenance.



Environmental significance

Maintenance and chemicals account for a large part of the cost in diverse technologies for water purification. Thus, a self-maintainable decentralized water treatment system with zero commercial chemicals is appealing for sustainable water cleanup, especially significant for rural areas. Solar-driven H2O2 production and in situ activation provide the possibility to develop an advanced oxidation process with zero chemicals and maintenance. We coupled photocatalytic H2O2 production and UVC activation in a flow-through operation for organic micropollutant removal in water. This process was realized by developing magnetic separable resorcinol–formaldehyde photocatalysts on Fe3O4@SiO2 microspheres, which can produce H2O2 solution by facile cycling of catalysts. This work provides a promising way to develop water purification processes with zero chemical addition and maintenance.

Introduction

Hydrogen peroxide (H2O2)-based advanced oxidation processes (AOPs) have been widely applied to remove persistent organic micropollutants in water by producing strong oxidative species like hydroxyl radicals (˙OH).1–3 Among these AOPs, ultraviolet (UV)/H2O2 is the most effective one to remove diverse organic pollutants just by using electrical energy (for UV light) and H2O2 to produce ˙OH at a high quantum yield (up to 100%).4–6 The cost of this process is the sum of electrical energy and oxidant costs, in which maintenance accounts for up to 45% of the electrical energy cost.7,8 A great number of efforts have been made to enhance the removal efficiency and decrease the operation cost by using additional chemicals (e.g. persulfate) and optimizing reactors.9–11 However, it would be effective to minimize the cost by developing a process that avoids chemical addition and maintenance. This is especially significant for decentralized water purification in rural areas.

The current commercial production of H2O2 is based on an anthraquinone process, which is limited by the costly hydrogen gas, noble metal catalysts, toxic organic solvents, and high-energy inputs.12,13 Moreover, the storage and transportation of the concentrated H2O2 (above 30%) is hazardous, and dilution is necessary in the further utilization for water purification.4,14 This makes the maintenance of the H2O2-involved processes inevitable. Photocatalytic H2O2 production by converting earth-abundant H2O and O2 over photocatalysts is an emerging approach to produce H2O2 at mild concentrations on a small scale.15–17 In this solar-to-chemical process, the two-electron oxygen reduction reaction (ORR) for H2O2 synthesis is enabled by photogenerated electrons, while water is oxidized by photogenerated holes and synchronously offers protons.18–20 Photocatalytic H2O2 production displays great potential for diverse water purification applications,21,22 while the development of efficient photocatalysts is the prerequisite to realize it. Among the photocatalysts for H2O2 production, the resorcinol–formaldehyde (RF) copolymer, a metal-free photocatalyst, possesses a narrow bandgap (2.0 eV) and a wide absorption region (up to 700 nm). Under sunlight irradiation, H2O2 can be produced over an RF copolymer in pure water with a relatively high solar-to-H2O2 conversion efficiency (0.5%).23,24 However, this RF material exhibits a form of powder with low density and poor dispersion, resulting in challengeable separation. Immobilizing the photocatalysts on porous substrates is one feasible choice but significantly decreases mass transfer and H2O2 production. The downstream separation such as membrane filtration is energy-costing, and organic membranes are labile in H2O2 solution.25,26 Thus, facile separation of photocatalyst powder to ensure production of a clean H2O2 solution is a prerequisite for the integration of H2O2 production and on-site utilization for water purification.

Magnetic nanomaterials such as Fe3O4 nanoparticles can be easily collected and recovered by using external magnetic fields, and the recovery of water can reach 100% after magnetic separation.27–29 These materials are usually used as catalyst supports to improve recyclability.8,30,31 Herein, we report a strategy to develop magnetic separable photocatalysts by in situ growing RF layers on silica-coated magnetite microspheres, and developed a process integrating photocatalytic H2O2 synthesis and on-site UVC activation to remove organic pollutants in water. This process displays great potential to be operated without any chemical addition and maintenance.

Experimental section

Synthesis of catalysts

Fe3O4 magnetic nanoparticles. Fe3O4 magnetic nanoparticles were synthesized by a solvothermal method.32 2.7 g of iron(III) chloride hexahydrate (98%, Sinopharm) and 7.2 g of sodium acetate (98%, Sinopharm) were dissolved in 100 mL of ethylene glycol (98%, Aladdin Biochemical Technology) and stirred for 10 min to form a clear yellow solution. Then, the homogeneous solution was transferred into a Teflon-lined stainless steel autoclave (100 mL) and heated at 200 °C for 8 hours. Then the autoclave was cooled down to room temperature, and the black product was washed with ethanol and water, separated and vacuum dried at 60 °C for 12 hours to obtain Fe3O4 magnetic nanoparticles.
Fe3O4@SiO2 microspheres. The Stöber method was employed to form a SiO2 layer over the Fe3O4 surface. The as-prepared Fe3O4 nanoparticles (0.10 g) were pre-treated in 50 mL hydrochloric acid solution (0.1 M) under 10 min ultrasonication. After washing and separation, the pre-treated Fe3O4, 1.5 mL ammonia solution (28 wt%, Sinopharm) and 1.86 g tetraethyl orthosilicate (TEOS, 98%, Aladdin Biochemical Technology) were added into 100 mL of 80 vol% ethanol solution, followed by stirring at room temperature for 360 min. Finally, Fe3O4@SiO2 microspheres were obtained after washing, filtering and drying under vacuum at 60 °C for 6 hours.
Magnetic resorcinol–formaldehyde photocatalysts. Fe3O4@SiO2 microspheres (0.1 g), ammonia (0.1 mL, 28 wt% Sinopharm) and cetyltrimethylammonium bromide (CTAB, 0.01 mmol, 99%, Sigma-Aldrich) were mixed in 30 mL of deionized water and stirred for 30 min. Then, 4.5 mmol of resorcinol (99%, Sigma-Aldrich) and 8.2 mmol of formaldehyde solution (33 wt%, Sinopharm) were added into the mixture and mechanically stirred for 16 hours. Then, the suspension was transferred into a Teflon-lined stainless steel autoclave (50 mL) and kept at 210 °C for 24 hours. The obtained black samples are magnetic resorcinol–formaldehyde catalysts, which were labeled as MRF. MRF-0.5 and MRF-2.0 were synthesized according to the same procedure as MRF, but the dosages of resorcinol and formaldehyde were half and double of those used in MRF synthesis, respectively. RF photocatalysts were prepared via the same procedure but without magnetic particles.

Characterization

The morphology of materials was recorded by using a Talos F200X scanning transmission electron microscope (TEM, FEI, USA). The accelerating voltage for each test is 200 kV. The X-ray diffraction (XRD) patterns of samples were collected on a Rigaku D/max-2200 PC X-ray diffractometer with Cu-Kα radiation (λ = 0.154 nm, 40.0 kV and 30.0 mA). The Fourier transform infrared (FTIR) spectra were recorded on a Thermo Electron Nicolet 6700 spectrometer. X-ray photoelectron spectra (XPS) were recorded on a Shimadzu-Kratos spectrometer (Al Kα radiation, 2 × 10−9 Pa) with an Axis Ultra DLD system. The BET specific surface area and pore volume analyses were carried out on a gas sorption analyzer (Quantachrome Autosorb-IQ3). Thermogravimetric analysis (TGA) and differential scanning calorimetry (DSC) were carried out on a Mettler-Toledo analyzer (TGA/DSC1/1600HT). The temperature is increased from 20 to 800 °C (10 °C min−1) in an air atmosphere (30 mL min−1). Magnetic properties of the materials were measured on a SQUID-based vibrating sample magnetometer (VSM, MPMS-3, Quantum Design) at room temperature.

Photocatalytic reaction

Photocatalytic H2O2 production was conducted in a 50 mL quartz cuvette. Typically, 30 mg of catalysts were dispersed in 30 mL of pure water. During the tests, a Xe lamp (PLS-SXE300, 300 W) with a cut-off filter (λ > 420 nm) provided visible-light irradiation, and the suspension was continuously purged with air. The dissolved O2 concentration was measured by using a fiber optic oxygen meter (OXY-1 SMA, PreSens Precision Sensing GmbH, Germany). The magnetic catalysts can be separated by using a magnet for the cycle tests. Photocatalytic H2O2 decomposition was carried out in a H2O2 suspension (1000 μM) containing 1 g L−1 of catalysts in a N2 atmosphere under visible-light irradiation (λ > 420 nm). The H2O2 concentration was determined by the N,N-diethyl-p-phenylenediamine (DPD, 97%)-horseradish peroxidase (POD, RZ > 1.5) method.33,34

Organic pollutants including rhodamine B (RhB), humic acid (HA) and tetracycline (TC) were degraded via a UVC/H2O2 coupling with photocatalytic H2O2 production. In a typical test, H2O2 was generated by using a 150 mL MRF suspension (1 g L−1) after 60 min visible light irradiation with air purging. Then, the catalysts were separated from water by using a magnetic field, and the H2O2 solution was used for wastewater treatment. Both batch and flow-through tests were carried out to evaluate organic degradation in the UVC/H2O2 processes. In a batch operation, 5 mL of H2O2 aqueous solution (100 μM) was mixed with 45 mL wastewater and irradiated under a UVC light for 60 min. The UVC light source was six G4T5 bulbs (Sankyo Denki, λ = 254 nm, 4 W). In a flow-through operation, 200 mL of H2O2 solution (100 μM) was mixed with 1800 mL of wastewater containing a certain concentration of organic micropollutants (RhB, HA or TC). Then, the mixture was pumped into a UVC reactor at 10, 20 or 30 mL min−1 flow rate. The section view of UVC reactor is shown in Fig. S1. A UVC lamp (Cnlight, λ = 254 nm, 15 W) was used and the effective volume for wastewater treatment was 1000 mL. The concentration of RhB, HA and TC was measured by using a UV-vis spectrophotometer (TU-1810, Beijing Purkinje) at 564, 254 and 357 nm, respectively. The electrical energy per order (EEO) in the flow-through operation is calculated using eqn (1):35

 
image file: d2va00228k-t1.tif(1)
where, P is the power of the UVC light (kW); F is the volume flow rate of water (m3 h−1); Ci and Cf are the initial and final concentrations of micropollutants (mg L−1), respectively.

Results and discussion

Characterization of MRF microspheres

The magnetic resorcinol–formaldehyde (MRF) photocatalyst was synthesized by the procedure described in Fig. 1A. Fe3O4 nanoparticles have superparamagnetism and have been frequently used as the magnetic core for magnetic separable core–shell materials. To prevent the aggregation and possible etching of Fe3O4 nanoparticles by reacting with H2O2,36 a layer of SiO2 coating is incorporated on the surface of Fe3O4 due to its good compatibility and hydrophilicity.37,38 However, under the alkaline conditions for the polycondensation of RF (pH > 10), the SiO2 layer would be negatively charged. Considering that the surface of RF particles is also negative,37 and electrostatic repulsive force between the two components would accordingly inhibit the formation of RF over SiO2, a cationic surfactant (CTAB) is employed to render the surface of silica layers positively charged. Thus, the RF shell layer eventually in situ formed over silica-coated Fe3O4 microspheres.
image file: d2va00228k-f1.tif
Fig. 1 (A) Schematic synthetic procedure of the magnetic resorcinol–formaldehyde photocatalysts; (B)–(D) TEM images of (B) Fe3O4 particles, (C) Fe3O4@SiO2 (inset: HRTEM image at the core–shell interface), and (D) MRF microspheres; (E) XRD patterns of MRF; (F) FTIR spectra of various materials; (G) high-resolution O 1s XPS spectrum of MRF.

As shown in Fig. 1B, Fe3O4 nanoparticles are prepared via a solvothermal method, and the as-synthesized spherical particles possess a mean diameter of 500 nm. Then, a silica layer about 50 nm of thickness is coated over the surface of Fe3O4 microspheres (Fig. 1C). No lattice fringe is observed in the SiO2 region (inset in Fig. 1C), indicating that the SiO2 layer is dominated by the amorphous phase.39,40 CTAB induces a positively charged surface of Fe3O4@SiO2, and then the RF copolymer as the shell layer is formed over Fe3O4@SiO2via a Stöber-like method.22,39 The thickness of this shell layer is about 100 nm (Fig. 1D).

The crystalline structure of the catalyst is determined using powder XRD patterns (Fig. 1E). The diffraction pattern of MRF matches well with the JCPDS card 19-0629 for the face-centered cubic Fe3O4 phase.41,42 The diffraction peaks at 30.2°, 35.6°, 43.3°, 57.2° and 62.8° correspond to the (220), (311), (400), (551) and (440) planes of cubic Fe3O4, respectively. A broad diffraction band at about 20° can be attributed to the (002) planes of graphitic carbon, suggesting the presence of π-stacking benzenoid–quinoid couples.22,43 The surface functional groups of MRF were also analyzed using FTIR spectra (Fig. 1F). The peak at 586 cm−1 corresponds to the stretching metal–oxygen vibration of the Fe–O groups.44,45 The weak bands at 798 and 956 cm−1 are assigned to the Si–O and Si–OH groups, respectively.46 The bands located at 1615 and 1450 cm−1 correspond to the stretching vibration of the aromatic C[double bond, length as m-dash]C and C–H groups of the methylene linker, respectively.47,48 The benzenoid–quinoid D−A resorcinol couples of the RF copolymer layers in MRF were proved by XPS spectra. The deconvoluted peaks in the C 1s (at 286.2 eV and 288.0 eV) (Fig. S2) and O 1s (at 533.0 eV and 531.4 eV) XPS spectra (Fig. 1G) are assigned to the C–O and C[double bond, length as m-dash]O bonds, corresponding to the benzenoid and quinoid forms in the RF framework, respectively.21 The ratio of C–O/C[double bond, length as m-dash]O obtained according to the data of the O 1s spectrum is 2.5. Thus, a shell of the RF copolymer was successfully formed over the Fe3O4@SiO2 cores.

Photocatalytic H2O2 production over MRF microspheres

Fig. 2A reveals the time-dependent H2O2 production in water over different materials under visible light. Fe3O4@SiO2 microspheres and Fe3O4 nanoparticles produce negligible H2O2, indicating that the support materials for RF have no photocatalytic activity. Using MRF (1 g L−1) as the photocatalyst, H2O2 concentrations increase linearly with time, achieving a H2O2 production rate of 100 μM h−1 under air purging conditions, in which the dissolved oxygen concentration is about 10 mg L−1. When the suspension is purged with O2, the dissolved O2 increases to about 40 mg L−1, and the photocatalytic H2O2 production within 60 min is enhanced to 150 μM. However, when purging with N2, the system produces negligible H2O2, suggesting that the oxygen reduction is the main pathway for H2O2 production.49–51 Upon 12 hours of irradiation under air purging conditions, MRF can produce 1200 μM H2O2 without any retardation (Fig. S3), which is a relatively high value in the systems of photocatalytic H2O2 production in the absence of any organic sacrificial agent (Table S1).
image file: d2va00228k-f2.tif
Fig. 2 (A) Photocatalytic H2O2 production over different materials (catalysts: 1 g L−1; pH = 7.5; λ > 420 nm; O2/air/N2: 0.5 L min−1); (B) TGA and DSC profiles for MRF pyrolysis; photocatalytic H2O2 production within 60 min (C) over different dosages of MRF and (D) over 1 g L−1 MRF at different pH values; (E) normalized H2O2 production over per gram of RF copolymers under air purging conditions; and (F) H2O2 decomposition over Fe3O4@SiO2 in the dark and under visible-light irradiation (catalysts: 1 g L−1; [H2O2]0: 1000 μM; pH = 7.5; λ > 420 nm; N2: 0.5 L min−1).

The ratios of RF to Fe3O4@SiO2 in MRF are optimized by measuring the performance of photocatalytic H2O2 production. The dosage of resorcinol and formaldehyde for MRF-0.5 and MRF-2.0 are 0.5-fold and 2.0-fold of that for MRF, respectively. As shown in Fig. S4, H2O2 production over MRF-0.5 is 0.8-fold of that of MRF, while this over MRF-2.0 is only a 10% increase by comparing with that produced by MRF, suggesting that the content of RF polymers in MRF is nearly enough for photocatalytic H2O2 production. Thus, MRF is used for further tests due to its ratio of RF to Fe3O4@SiO2 being optimal.

The weight percentage of the RF polymer in MRF was measured by the TGA-DSC analysis under air purging conditions (Fig. 2B). A two-stage weight loss can be observed in the TGA curve. Below 300 °C, weight loss is less than 3%, which can be ascribed to the removal of moisture in the materials. In the range of 300–550 °C, the weight loss is about 32%, accompanied by two exothermic peaks at 325 and 530 °C. This is associated with the decomposition of the RF polymer. When the temperature increases to above 550 °C, the weight percentage of MRF remains at 65%, corresponding to the inorganic component in the material. Thus, considering 65% inorganic components and 3% moisture in the material, the weight percentage of the RF copolymer in MRF is about 32%. According to the N2 adsorption/desorption isotherm and the pore-size distribution curves of MRF (Fig. S5), the specific surface area and total pore volume of this catalyst are 16.0 m2 g−1 and 5.3 × 10−2 cm3 g−1, respectively. This indicates that MRF is a nonporous material, and the photocatalytic ORR mainly takes place over the surface layer.

H2O2 production increases with the increase of MRF dosages in the suspension (Fig. 2C). In the presence of 5 g L−1 and 10 g L−1 of MRF, the produced H2O2 in 60 min reaches 200 and 250 μM, respectively. H2O2 production on MRF shows a minor decrease with the increase of pH from 3 to 9, while above 80 μM upon 60 min irradiation at all the pH values (Fig. 2D). These results suggest that MRF displays a high and stable activity over a wide pH range, and continuous photocatalytic H2O2 production in pure water can be achieved by using a high dosage of MRF.

Considering that the weight percentage of RF in MRF is about 32%, the H2O2 production rate is normalized according to the weight of the RF copolymer, and the results are shown in Fig. 2E. In a control test, the pristine RF copolymer produces 300 μM H2O2 in 60 min, which is 3-fold that on MRF under the same conditions (Fig. S6). Thus, the normalized H2O2 production of MRF is close to the theoretical value based on the pristine RF copolymer (Fig. 2E), suggesting negligible H2O2 decomposition on the Fe3O4@SiO2 component in MRF microspheres. This is further proved by measuring H2O2 decomposition over Fe3O4@SiO2 under both dark and illumination conditions. As shown in Fig. 2F, in the N2-purging Fe3O4@SiO2 suspension, H2O2 concentration declines less than 2%, indicating that the as-prepared magnetic support materials do not consume H2O2 and affect H2O2 production. This is attributed to the tight layers of RF and SiO2 blocking the access of H2O2 to core materials.28,38

The magnetization properties of materials are proved by VSM analysis. As shown in the magnetic hysteresis loops (Fig. 3A), the saturation magnetization (Ms) values for Fe3O4, Fe3O4@SiO2 and MRF are 80.5, 60.6 and 59.9 emu g−1, respectively. Moreover, negligible remanence or coercivity of all the curves are detected, proving the super-paramagnetism of these materials. As a result, MRF particles that disperse well in water can be rapidly aggregated in the presence of an external magnetic field (inset in Fig. 3A), and the recovery of MRF is over 99%. The characters and photocatalytic activity of the reused MRF after 12 h of prolonged irradiation were measured. As shown in the XPS spectrum of recovered MRF after the photocatalytic reaction (Fig. S7), the changes of the band for the C[double bond, length as m-dash]O bond are negligible. The TEM (Fig. S8) and FTIR spectra (Fig. 3B) are almost the same as those of the fresh materials, indicating that the changes of the functional groups and microstructures of MRF are negligible. After five-cycle experiments, the H2O2 yield and the saturation magnetization of MRF (1 g L−1) remain at 100 μM h−1 and 59.6 emu g−1 (Fig. 3C and D). The recovered MRF maintains the activity for H2O2 production and the magnetization for rapid separation. The total organic carbon (TOC) of the solution after removing MRF was 0.5 mg L−1, which is almost the same as that of the control of deionized water, suggesting that the organic components in the material scarcely dissolve. Thus, the MRF photocatalysts display superior stability and easy recyclability, which enables ready utilization of the produced H2O2 for on situ usage.


image file: d2va00228k-f3.tif
Fig. 3 (A) Magnetic hysteresis loops of the catalysts at room temperature and (A inset) magnetic separation and redispersion process of MRF; (B) FTIR spectra of MRF and reused MRF; repeated photocatalytic H2O2 production (C) and magnetic hysteresis loops (D) of reused MRF (catalysts: 1 g L−1; pH = 7.5; λ > 420 nm; air: 0.5 L min−1).

On situ H2O2 utilization for decontamination via UVC irradiation

A process combining H2O2 production and on situ utilization for organic micropollutant removal is proposed (Scheme 1). In one cycle of the test, MRF (150 mg) is firstly dispersed in water (150 mL) by purging with air (I). Then, upon visible light irradiation, free electrons and holes are generated for the two-electron ORR and four-electron WOR, respectively (II). In this step, about 100 μM of H2O2 is produced per hour. Subsequently, MRF particles rapidly aggregate under the magnetic field and get separated from the H2O2 solution. After withdrawing the magnetic field, the catalysts are re-dispersed in fresh water and are ready for the next cycle (III). After three cycles, about 400 mL of the H2O2 solution at 100 μM concentration (40 μmol of H2O2) can be collected. The major energy consumption in photocatalysis comes from a 300 W xenon lamp, which can be conveniently replaced by sunlight. The H2O2 solution generated from photocatalysis mixes with the micropollutant-containing wastewater, and is then treated by UVC light irradiation through a batch or a flow-through operation.
image file: d2va00228k-s1.tif
Scheme 1 Schematic illustration of sequencing batch photocatalytic H2O2 production over MRF (A) and UVC/H2O2 flow-through processes (B) for organic micropollutant degradation.

In the batch operation, 5 mL of H2O2 solution (100 μM) was added into 45 mL of wastewater, resulting in the initial H2O2 and pollutant (RhB, HA, or TC) concentrations of 10 μM and 1 mg L−1, respectively. The wastewater containing H2O2 was irradiated by using UVC light for 60 min. As shown in Fig. 4A, under dark conditions, the reduction of RhB, HA, and TC in the presence of 10 μM H2O2 is negligible. In the absence of H2O2 but upon UVC irradiation alone for 60 min, HA and TC have negligible reduction, while RhB has about 33.1% reduction. However, in the UVC/H2O2 system, the concentrations of RhB, HA and TC decrease to 0.05, 0.15 and 0.2 mg L−1 in 60 min, respectively. Owing to the UVC-induced H2O2 activation, hydroxyl radicals are produced to oxidize these organic pollutants.52,53 The decay curve exhibits first-order reaction kinetics, and the rate constants for RhB, HA and TC are 0.045, 0.035 and 0.027 min−1, which are about 6.7, 52.6 and 34.6-fold values of that treated by UVC irradiation in the absence of H2O2, respectively (Fig. S9). The performance of RhB degradation via a sequencing batch process scarcely declines even after five cycles (Fig. 4B), indicating that this process exempted from external chemicals is robust to remove organic micropollutants in water.


image file: d2va00228k-f4.tif
Fig. 4 (A) The removal of RhB, TC and HA via UVC/H2O2, UVC and H2O2 processes in batch tests; and (B) recyclability of the process for RhB removal (RhB, TC or HA: 1 mg L−1; H2O2: 10 μM).

In a flow-through operation, 1 mg L−1 of RhB (HA or TC) wastewater containing 10 μM of H2O2 produced from MRF photocatalysis were pumped into a UVC reactor at a 10 mL min−1 flow rate. The retention time for the wastewater is 100 min. As shown in Fig. 5, under UVC irradiation or H2O2-alone treatment, the RhB concentration in the effluent is about 0.20 and 0.99 mg L−1. The significant removal of RhB by UVC irradiation alone in the flow-through operation can be attributed to the prolonged irradiation time. However, upon UVC irradiation, the RhB concentration in the H2O2-containing water decreases to below 0.01 mg L−1, and the pink wastewater completely bleaches. The treatment also achieves high removal efficiencies for HA- or TC-containing wastewater. Without light or H2O2, negligible micropollutants (less than 5%) are decomposed. In the UVC/H2O2 system, the HA and TC concentrations in the effluent decrease to 0.35 and 0.20 mg L−1, respectively. As the flow rate of water increases, the removal efficiency of micropollutants decreases (Fig. 5B). At 30 mL min−1 of flow speed, the RhB, HA and TC concentrations in the effluents are 0.15, 0.75 and 0.75 mg L−1, respectively. This can be attributed to the less residence time caused by the higher flow rates. It can be expected that the removal efficiencies can be further enhanced by increasing the H2O2 dosages. The EEO values of the pollutant decomposition in the flow-through operation are calculated according to eqn (1).7,35 As shown in Fig. 5C, the EEO values for the three pollutants are 10–60 kW h m−3 per order, which is comparable to the values in photo-Fenton and UV/peroxydisulfate systems (Table S2). Considering that the electrical energy required for both H2O2 production and UVC/H2O2 processes can be replaced by sunlight and solar cells, it is promising to minimize the energy consumption in H2O2 production and activation. Thus, the process of coupling photocatalytic H2O2 production and on-site H2O2 activation by using UVC has great potential to be automatically operated outdoor, featuring minimum energy input, and zero maintenance and chemical addition.


image file: d2va00228k-f5.tif
Fig. 5 (A) The concentration of micropollutants in the effluent via a flow-through operation (RhB, TC or HA: 1 mg L−1; H2O2: 10 μM; flow rate: 10 mL min−1; λ = 254 nm); (B) the concentration of micropollutants in the effluent via a flow-through operation at different flow rates; (C) EEO value of RhB, HA and TC decomposition in a flow-through operation (RhB, TC or HA: 1 mg L−1; H2O2: 10 μM; λ = 254 nm).

Conclusions

In summary, we developed a zero-chemical process to remove organic micropollutants in water via integrating H2O2 production by photocatalysis and activation by using UVC. A magnetic core–shell photocatalyst was fabricated by in situ growth of resorcinol–formaldehyde copolymers over silica-coated Fe3O4 microspheres, which can achieve 100 μmol h−1 H2O2 production from water and air over per gram MRF in the absence of organic sacrificial agents. This magnetic material can be easily separated and recycled. A UVC/H2O2 operation was developed by continuously mixing wastewater and the generated H2O2 solution, and then flowing it through a UVC reactor, which can efficiently activate H2O2 and degrade organic micropollutants. The process only needs light as energy input and water and air as the raw materials, representing a low-cost route to convert solar energy for environmental cleanup.

Author contributions

J. Z., Q. Z. and X. Z. designed and performed the experiments. J. Z. wrote the original draft. C. C. performed the photocatalytic performance analysis. X. G. wrote and revised the manuscript. M. L. conceived the original idea, supervised the project, and revised the manuscript.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

This work was supported by the National Natural Science Foundation of China (nos 52070128 and 22111530110).

Notes and references

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Footnote

Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2va00228k

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