Home Optimized Cu2O-{100} facet for generation of different reactive oxidative species via peroxymonosulfate activation at specific pH values to efficient acetaminophen removal
Article Open Access

Optimized Cu2O-{100} facet for generation of different reactive oxidative species via peroxymonosulfate activation at specific pH values to efficient acetaminophen removal

  • Ke Chen , Xudong Yang , Rui Hao , Minghui Shao , Xiaoyong Yang , Xiuze Li , Yuxuan Li , Juzhe Liu and Sai Zhang EMAIL logo
Published/Copyright: June 14, 2023
Become an author with De Gruyter Brill

Abstract

Activation of peroxymonosulfate (PMS) to degrade persistent organic contaminants has received increasing attention in wastewater purification. In this study, Cu2O catalysts with different exposed crystal facets were prepared, characterized, and evaluated for acetaminophen (ACE) degradation through PMS activation. The experimental results showed that cubic Cu2O with {100} facets exhibited remarkable activity on ACE removal by PMS activation in wide pH range of 3–11. DFT calculations indicated that Cu2O-{100} displayed higher electron transfer efficiency and PMS adsorption ability, further improving PMS activation. The radicals quenching experiments and electron paramagnetic resonance (EPR) results illustrated that singlet oxygen (1O2) was dominant reactive oxidative species (ROSs) during oxidation reactions and the relevant generation pathways were distinctly elucidated. Finally, the possible PMS activation mechanisms were discussed for ACE degradation in a wide pH range. This study will provide new insights to disclose PMS-based advanced oxidation processes (AOPs), and offer a new approach for wastewater purification by non-radical reactions.

1 Introduction

Recently, pharmaceutical and personal care products (PPCPs) detected in water bodies are posing serious threat to people’s health. As one of the typical PPCPs, acetaminophen (ACE) has been heavily applied to treat fever and relieve pain, which can be discharged into the surroundings by various paths and will endanger water circumstances and human bodies [1]. However, the removal of ACE from waste water is difficult to achieve through traditional sewage treatment processes due to its trace-level concentration and complex structure. Accordingly, it is quite essential to seek for advanced degradation systems and techniques to remove ACE from water.

Sulfate radical-based advanced oxidation processes (SR-AOPs) have been considered as the most promising processes to effectively remove refractory organic pollutants from wastewater. Various radicals and non-radials, such as sulfate radicals (SO4˙), hydroxyl radicals (˙OH), and singlet oxygen (1O2), are generated by activation of persulfate (PS, S 2 O 8 2 ) or peroxymonosulfate (PMS, HSO 5 ) during SR-AOPs, which mostly possess strong oxidized ability to achieve complete degradation of pollutants [2,3]. In general, PS and PMS can be activated with diversified degradation mechanisms via metal-based catalysts, thermal treatment, ultraviolet/alkali activation, and supersonic wave, which make it more difficult to control [3,4]. Meanwhile, water quality parameters (such as solution pH, impurity ions, and natural organic matter [NOM]) also influence the activation of PS/PMS, thereby, influencing pollutant degradation during water treatment. For instance, the formation and species of reactive oxidative species (ROS) are greatly dependent on solution pH [5]. Additionally, SO4˙ possesses a higher oxidation potential in contrast to conventional ˙OH under neutral pH, while SO4˙ and ˙OH display similar oxidation abilities in acidic condition [6]. Most of all, the reasonable design of metal-based catalysts, as the key factor for PMS activation, can optimize the degradation process with improved degradation rate [5]. Over the past decade, many strategies such as morphology/structure control, facet engineering, fabricating heterojunction, and element doping have been employed to achieve highly efficient catalysis [2,7]. For instance, the catalytic performances of Co3O4 catalysts in heterogeneous system for PMS activation depend on their morphologies and structures (e.g., nanospheres, nanotubes, nanorods, nanosheets, nanorings, etc.) [8]. Specifically, the crystal facets regulation is to change the exposed facets of catalysts with different geometric and electron structure. Precise regulation of crystal facets greatly improves catalytic activities and electron structure properties of catalysts [9]. On one hand, different crystal facets have different electron transfer rates and thus influence oxidation/reduction potentials. On the other hand, different crystal facets with different atomic arrangement and dangling bonds can alter the adsorption energy of target organic compounds on catalyst, consequently affecting its catalytic activities. For instance, Wu et al. reported that preferential growth of the cobalt (200) in Co@N–C exhibited excellent catalytic activities for PMS activation on the removal of bisphenol A [7]. Similarly, Hao et al. demonstrated that Fe(ii) on the {001} facets of hematite possessed a higher reactivity and electron transport efficiency than that on the {110} facets [9].

Of the various catalysts available to date, cuprous oxide (Cu2O) is easy to realize exposed facet regulation, which also owns inherent advantages including low cost, excellent electron transport properties, and unique structures [10]. Most importantly, it has been reported that Cu2O is a typical non-radical mechanism catalyst to efficiently activate PMS for organic pollutants degradation. Therefore, it is very important to develop tunable crystal facets of Cu2O to realize highly efficient catalysis, clarify the effect of different exposed facets on catalysis, and unveil the activation mechanism under different water qualities, but the related research is yet ambiguous. Thus, it is essential to design Cu2O catalysts with superior exposed specific facets for SR-AOPs in wastewater treatment and disclose the mechanism of ROS generation induced by Cu species for better catalytic activity.

Herein Cu2O catalysts with different exposed facets are successfully synthesized, and certain characterizations have been conducted to verify their microscopic structure, which exhibits excellent degradation performances for ACE removal via PMS activation. The specific objectives are to: (i) develop Cu2O catalysts with different exposed facets for ACE degradation via PMS activation, and investigate the influences of solution pH on ACE removal, (ii) clarify the structure–activity relationship of Cu2O with different exposed facets and HSO 5 by density functional theory (DFT) calculations, (iii) identify the main ROSs during reactions under different solution pH via quenching tests and electron paramagnetic resonance (EPR) analysis, (iv) explore the changes of Cu species affected by various pH, and (v) elucidate the mechanism for enhanced organic pollutants degradation by PMS activation. This work can deepen the understanding of PMS activation induced by Cu-based catalysts and will provide a new direction for non-radical processes in wastewater treatment.

2 Experimental method

2.1 Materials

ACE (98%, C8H9NO2) was purchased from Innochem (Beijing, China). PMS was acquired from Alfa Aesar (Shanghai, China). Sodium hydroxide (NaOH), perchloric acid (HClO4), ethanol (EtOH, C2H6O), tert-Butanol (TBA, C4H10O), and ascorbic acid (C6H8O6) were acquired from Xilong Scientific Co., Ltd (Guangdong, China). Sodium thiosulfate pentahydrate (Na2S2O3·5H2O) was purchased from Beijing Tongguang Fine Chemical Company (Beijing, China). Methanol (CH3OH) was obtained from EMD Millipore Corporation (Shanghai, China). Formic acid (CH2O2) and polyvinylpyrrolidone (PVP) (K30, average molecular weight: 40,000) were bought from Aladdin Reagent Co., Ltd (Shanghai, China). Deionized water used in the experiment was acquired from Beijing Zhongjing Keyi Technology Co., Ltd (Beijing, China).

2.2 Preparation of Cu2O with different crystal faces

The synthesis routes followed the previous report with minor modification [10]. Typically, 0.171 g of CuCl2·2H2O and certain polyvinylpyrrolidone (PVP, K30) (0 g for cubic Cu2O, 1.5 g for vertex-truncated Cu2O, and 4.5 g for octahedral Cu2O) were mixed in 100 mL of deionized water. After stirring for 10 min and ultrasonication for 20 min, 10 mL of NaOH aqueous solution (2 mol/L) was quickly added into the above solution to form a dark brown solution, and the mixture was continuously stirred for 30 min. Subsequently, 10 mL of ascorbic acid solution (0.60 mol/L) was added dropwise into the suspension, and then the mixture was aged for 3 h. Above procedures were performed under constant stirring except for special mention and heated in a water bath at 55°C. The final products were obtained after washing with absolute ethanol and water, and then dried under vacuum at 60°C for 12 h.

2.3 Characterization techniques

The surface morphologies of as-obtained samples were observed using environmental scanning electron microscopy (ESEM, FEI, Quanta 250 FEG). Transmission electron microscopy (TEM) and high-resolution TEM (HRTEM) images were observed on a Tecnai 30 FEG transmission electron microscope (FEI, USA, operating voltage 300 kV) to identify the microstructures of different samples. The powder X-ray diffraction (XRD) technology was performed to determine the crystal textures (DMAX-2400 by Japan Rigaku Company) with scanning diffraction angle (2θ) of 10–80° and 5°/min. X-ray photoelectron spectroscopy (XPS) was applied to explore the element composition (Axis Ultra multi-function electronic spectrometer manufactured by Kratos Analytical Ltd). The combined energy could pass the sample C1s peak fixed at 284.8 eV for calibration.

2.4 Degradation of ACE

Degradation experiments of ACE by PMS activation were conducted to evaluate the catalytic performances of different Cu2O catalysts. Typically, 100 mL of water and 100 µL of PMS solution (100 mmol/L) were mixed in a 250 mL beaker under magnetic stirring. The initial solution pH was adjusted to 5.0 ± 0.2 by using NaOH and HClO4. Subsequently, 1 mL of ACE solution (1 mmol/L) was placed into the above solution. After stirring for 5 min, 10 mg of catalysts was added into the mixture to start the degradation reaction. At given time intervals, 1 mL of reaction suspension was taken and immediately filtrated via a NYLON 0.22 μm syringe filter, which was quickly mixed with 100 μL of Na2SO3 solution (100 mmol/L) to quench the active radicals. The concentrations of ACE were detected on the Agilent Technologies 1260 Infinity II High Performance Liquid Chromatography (HPLC, Agilent 1260 Infinity II, USA) at the wavelength of 272 nm. The injection volume was 10 μL, and the flow rate was 1 mL/min. The separation was performed on an Agilent Zorbax SB-Aq (4.6 mm × 250 mm, 5 μm) liquid chromatography column. The temperature of the oven was controlled at 30°C, and the mobile phase was a mixture of methanol/0.1% formic acid solution (40/60%, v/v).

Effects of initial solution pH (from 3 to 11) on ACE degradation and quenching experiments by adding the tert-butanol (TBA, quenching ˙OH radicals, 100 mmol/L), ethanol (EtOH, quenching SO4˙ and ˙OH radicals, 100 mmol/L), and furfuryl alcohol (FFA, quenching singlet oxygen 1O2, 100 mmol/L) into the reaction system were also discussed. EPR technology was also used to identify SO4˙, ˙OH, and 1O2 active species with 5,5-dimethyl-1-pyrroline N-oxide (DMPO) and 4-amino-2,2,6,6-Tetramethylpiperidine (TEMP) as the spin-trapping agents, which was performed at room temperature on a Bruker A300 EPR spectrometer.

To investigate the reusability of cubic Cu2O, the used catalyst after the first cycle of ACE degradation by PMS activation was filtrated by a 0.22 μm PTFE membrane and then washed for the next cycling test. In this work, the relationship between the pseudo-first order kinetic rate constant (k 1) and the concentration of ACE was expressed by equation (1) as follows:

(1) ln ( C 0 / C t ) = k ,

where C 0 is the concentration at initial time, and C t is the concentration at reaction time. k 1 (min−1) and t are the pseudo first-order kinetic rate constant and the reaction time (min), respectively.

2.5 DFT calculation

The total DFT calculations were performed using the Vienna ab initio simulation package (VASP) with the projected augment wave pseudopotential [11,12]. The Perdew-Burke-Ernzerhof (PBE) exchange correlation function of the generalized gradient approximation was used to optimize the structures and obtain free energetics of small molecules [13,14]. For Cu2O-{100} and Cu2O-{111}, we used a 2 × 2 supercell in the lateral plane and the two-dimensional Brillouin zone was sampled with a 7 × 7 k-grid mesh. While, a Monkhorst-Pack k-point net of 3 × 3 was used after absorbing small molecules. A vacuum layer of 20 Å was applied above all Cu2O slab to avoid periodic interactions. The atomic positions were fully relaxed using the conjugated gradient method for energy minimization until calculated force on each atom was smaller than 0.01 eV/Å. The DFT-D3 method by Grimme was also employed to consider the long-range attractive van der Waals forces in the systems [15]. The adsorption energy was calculated using equation (2) as follows:

(2) E ads = E tot E bads E adsm ,

where E ads is the adsorption energy, E tot represents the total energy of the system after adsorption, E bads represents the total energy of the system before adsorption, and E adsm represents the energy of the adsorbed small molecule. If E ads < 0, it means that small molecules are easily adsorbed onto the surface of catalysts. In reverse, if E ads > 0, small molecules are hardly adsorbed onto the surface of catalysts.

The charge difference distribution (CDD) was obtained as follows:

(3) ρ diff = ρ tot ρ sub ρ HSO 5 ,

where ρ tot, ρ sub, and ρ HSO5 are the charge densities of HSO 5 /Cu2O-{100} or HSO 5 /Cu2O-{111}, pure Cu2O-{100} or Cu2O-{111}, and isolated HSO 5 molecule, respectively.

3 Results and discussion

Figure 1(a1–c1) and (a2–c2) displayed the ESEM images of Cu2O catalysts with typical cubic, vertex-truncated octahedral, and octahedral structures, which were obtained with the amount of PVP increased. Obviously, all these catalysts owned the quite uniform size of about 700 nm, and their corresponding three-dimensional models are provided in the insets of Figure 1(a2–c2). The exposed surfaces of the cubes, vertex-truncated octahedrons, and octahedrons were enclosed of six {100} facets, six {100} and eight {111} facets, and eight {111} facets (Figure 1(a2–c2)), which could be verified by the lattice fringes in the HRTEM images (Figure 1(a3–c3)).

Figure 1 
               Morphology characterization of Cu2O catalysts. The SEM images of the (a1 and a2) cubic Cu2O, (b1 and b2) vertex-truncated Cu2O, and (c1 and c2) octahedral Cu2O, and insets were the corresponding three-dimensional models. HRTEM images of (a3) cubic Cu2O, (b3) vertex-truncated octahedron Cu2O, and (c3) octahedral Cu2O.
Figure 1

Morphology characterization of Cu2O catalysts. The SEM images of the (a1 and a2) cubic Cu2O, (b1 and b2) vertex-truncated Cu2O, and (c1 and c2) octahedral Cu2O, and insets were the corresponding three-dimensional models. HRTEM images of (a3) cubic Cu2O, (b3) vertex-truncated octahedron Cu2O, and (c3) octahedral Cu2O.

To study the structural information and surface chemical state, XRD and XPS spectra of as-obtained catalysts were measured. As displayed in Figure 2, several apparent diffraction peaks at 29.5°, 36.4°, 42.3°, and 61.3° were observed for all samples, corresponding to the (110), (111), (200), and (220) planes of cuprite Cu2O (JCPDS No. 77-0199) [10]. Moreover, the XPS survey spectra of different samples in Figure S1a confirmed the existence of Cu and O in all the three Cu2O catalysts. By comparison, more active Cu atoms were exposed on the surface of cubic Cu2O with a Cu/O atomic ratio of 0.99, which was higher than that of vertex-truncated Cu2O (0.66) and octahedral Cu2O (0.58). This probably resulted from the difference in their exposed crystal facets, which then induced the different PMS activation performances during reactions [8]. In Figure S1b, two peaks were observed for the high-resolution spectra of O 1s at 530.5 and 531.4 eV, assigned to the lattice oxygen and surface adsorbed H2O, respectively [16,17]. The core-level Cu 2p spectrum in Figure S1c exhibited two dominant peaks centering at 932.7 and 952.4 eV, which belonged to Cu 2p3/2 and Cu 2p1/2 of Cu+ [18]. Besides, two weak peaks at 934.7 and 955.2 eV were assigned to Cu2+, which might be resulted from slight oxidation of Cu2O [16].

Figure 2 
               XRD patterns of cubic, vertex-truncated, and octahedral Cu2O catalysts.
Figure 2

XRD patterns of cubic, vertex-truncated, and octahedral Cu2O catalysts.

The degradation of ACE was investigated through PMS activation over different catalysts. As displayed in Figure 3a, the concentration of ACE was not decreased after adsorption for 10 min, which suggested that the cubic Cu2O had no capacity to adsorb ACE. Meanwhile, the control experiment with only PMS addition indicated that PMS could not degrade ACE directly. However, an obvious removal of ACE was observed after adding cubic Cu2O catalyst with admirable efficiency of 100% in 7 min. In contrast, octahedral Cu2O and vertex-truncated octahedral Cu2O exhibited inferior degradation efficiency of 88.23 and 94.55% in 10 min, respectively. Pseudo first-order kinetic rate constants (k 1) of ACE degradation over various catalysts were evaluated and demonstrated in Figure 3b. The relevant k 1 of cubic Cu2O was 0.61 min−1, which was 1.74 and 2.65 times of vertex-truncated octahedral (0.35 min−1) and octahedral Cu2O (0.23 min−1), verifying its higher kinetic reaction rate. These results illustrated that cubic Cu2O possessed superior ability to activate PMS and thus improved the oxidation degradation of refractory organic contaminants.

Figure 3 
               (a) Different catalyst-PMS systems for ACE removal and (b) the corresponding pseudo first-order kinetic model fitting. (c) The influence of different pH on ACE removal over cubic CuO2 by PMS activation and the inset was the corresponding degradation efficiency with 10 min. Influences of (d) Cl−, (e) coexisting cations, and (f) HA on ACE removal in various cubic CuO2 systems. Reaction conditions: [ACE]0 = 10 μmol/L, [PMS]0 = 100 μmol/L, [catalyst]0 = 0.1 g/L, [Cl−] = 1–10 mmol/L, [cation] = 2 mmol/L, [HA] = 0.25–1.0 mg/L, and solution pH 5.0 ± 0.2.
Figure 3

(a) Different catalyst-PMS systems for ACE removal and (b) the corresponding pseudo first-order kinetic model fitting. (c) The influence of different pH on ACE removal over cubic CuO2 by PMS activation and the inset was the corresponding degradation efficiency with 10 min. Influences of (d) Cl, (e) coexisting cations, and (f) HA on ACE removal in various cubic CuO2 systems. Reaction conditions: [ACE]0 = 10 μmol/L, [PMS]0 = 100 μmol/L, [catalyst]0 = 0.1 g/L, [Cl] = 1–10 mmol/L, [cation] = 2 mmol/L, [HA] = 0.25–1.0 mg/L, and solution pH 5.0 ± 0.2.

Since the generation of ROS was closely depended on the reaction system pH, we evaluated the effects of different initial solution pH on ACE degradation using cubic Cu2O as targeted catalyst. As shown in Figure 3c, cubic Cu2O exhibited the satisfactory degradation efficiency for ACE over a wide pH range from 3 to 11. Specially, ACE could be almost completely eliminated from the solution at pH 3, 5, and 11. Thus, the desired cubic Cu2O could work as a Janus catalyst in both acid and alkaline solvent environment.

Subsequently, the influences of co-existing ions and NOM on ACE degradation were also explored (Figure 3d–f). It could be noted that the degradation rate of ACE gradually increased with the Cl concentrations increasing from 1 to 10 mmol/L (Figure 3d). This was because the Cl anions might react with HSO 5 /SO4˙/˙OH to yield active chlorine species, such as HClO, ClO˙, and Cl˙, which possessed high selectivity and preferred to react with electron-rich moieties containing anilines, phenols, and olefins, thereby resulting in strong oxidation capacity for ACE removal [19]. As observed from Figure 3e, Na+ and Mg2+ ions showed no obvious effect during degradation reactions. However, the ACE degradation rate was inhibited by Ca2+ ions, which resulted due its electrical double layer compression effect and ion exchange capacity [20]. Figure 3f displayed that the ACE degradation efficiency decreased as the humic acid (HA) concentration increased from 0.25 to 1 mg/L, which was due to the fact that HA was a quencher of free radicals. Thus, cubic Cu2O with exposed {100} facets exhibited preferable degradation efficiency and significant adaptation in wide pH range as well as high salt condition.

To unveil the high activity from cubic Cu2O and clarify the roles of different exposed facets on PMS activation, DFT calculation was performed. As shown in the insets of Figure 4a and b, structural optimizations of bulk Cu2O were conducted, and two representative models with {100} and {111} exposed facets were obtained, which were denoted as Cu2O-{100} (cubic Cu2O) and Cu2O-{111} (octahedral Cu2O). Correspondingly, the electronic densities of state (DOS) for the two different models were also displayed in Figure 4a and b. Interestingly, the charge density state of Cu2O-{100} was across the Fermi level, suggesting its metallic property and superior electron transfer efficiency. While, the DOS spectra of Cu2O-{111} belonged to the characteristic feature of semiconductor, thus resulting in the decrease in conductive carriers. That is, rational morphology control effectively regulated the electron migration in cubic Cu2O with {100} exposed facets, which promoted the conductivity performance and interfacial reactions. The electron transfer property was further proved by electrochemical impedance spectroscopy in Figure S2, of which the semicircle diameter for cubic Cu2O was smaller than that of octahedral Cu2O and vertex-truncated Cu2O, indicating that the {100} facet for cubic Cu2O benefited for lowering the electron transfer resistance. Besides, the d-band center of Cu2O-{100} was calculated to be −2.27 eV, while it shifted to −2.37 eV for Cu2O-{111} after forming octahedral structure, hinting that the stronger adsorption ability of Cu2O-{100} for HSO 5 than that of Cu2O-{111}.

Figure 4 
               The DOS and atomic structure models of (a) Cu2O-{100} and (b) Cu2O-{111}. The DOS of (c) Cu2O-{100} and (d) Cu2O-{111} after adsorbing 
                     
                        
                        
                           
                              
                                 HSO
                              
                              
                                 5
                              
                              
                                 −
                              
                           
                        
                        {\text{HSO}}_{5}^{-}
                     
                   molecules. The adsorption energy and CDD for 
                     
                        
                        
                           
                              
                                 HSO
                              
                              
                                 5
                              
                              
                                 −
                              
                           
                        
                        {\text{HSO}}_{5}^{-}
                     
                   on (e) Cu2O-{100} and (f) Cu2O-{111}, respectively. The dark yellow and cyan regions represented the electron accumulation and charge depletion, respectively.
Figure 4

The DOS and atomic structure models of (a) Cu2O-{100} and (b) Cu2O-{111}. The DOS of (c) Cu2O-{100} and (d) Cu2O-{111} after adsorbing HSO 5 molecules. The adsorption energy and CDD for HSO 5 on (e) Cu2O-{100} and (f) Cu2O-{111}, respectively. The dark yellow and cyan regions represented the electron accumulation and charge depletion, respectively.

Furthermore, DFT calculations were employed to investigate the interaction between HSO 5 and Cu2O catalysts with different facet surfaces. It could be observed from Figure 4c that, after adsorbing HSO 5 molecules, no obvious change across the Fermi level was found for Cu2O-{100}, demonstrating that the extraordinary electrical conductivity of cubic Cu2O still remained. This meant that HSO 5 molecules as electron acceptors could effectively capture electrons from cubic Cu2O and be activated to produce sufficient radicals for pollutant degradation. With regard to Cu2O-{111}/ HSO 5 in Figure 4d, the obvious hybridization between O-p and Cu-4d orbitals occurred at the Fermi energy, which was beneficial for accelerating electron transport during the HSO 5 adsorption process. Moreover, charge density difference (CDD) and the Bader charge analysis were carried out to deeply elucidate the surface electron transfer mechanism. After adding HSO 5 molecules, the adsorption geometry structures of Cu2O-{100}/ HSO 5 and Cu2O-{111}/ HSO 5 were optimized and presented in Figure 4e and f. The adsorption energy of Cu2O-{100} for HSO 5 (−4.21 eV) was much higher than that of Cu2O-{111} (−3.06 eV), suggesting the superior adsorption ability of Cu2O-{100} toward HSO 5 , which was consistent with the d-band center results. Note that the charge depletion (the cyan region) occurred between the Cu–O and S–O bonds, while the electron accumulation (the dark yellow region) emerged around the bottom three O atoms in HSO 5 , resulting in an efficient activation of PMS on the surface of Cu2O. According to the Bader topological calculation, it was found that HSO 5 molecule captured 2.09 e and 1.99 e from the substrate Cu2O-{100} and Cu2O-{111}, respectively. This phenomenon indicated that valence electrons on cubic Cu2O could be effectively separated and transferred to bond with HSO 5 . Correspondingly, the O–O bond length of HSO 5 on Cu2O-{100} (1.473 Å) was slightly increased than that on Cu2O-{111} (1.467 Å). These findings confirmed that HSO 5 molecules were preferably activated by cubic Cu2O to generate more ROS. Therefore, DFT calculation results proved that Cu2O-{100} could provide more fluent electron transfer and contribute to PMS activation for improving the catalytic activity.

To unveil degradation mechanism of ACE in cubic Cu2O/PMS system at different initial pH, quenching experiments were carried out to confirm the major ROS generated in suspension during ACE oxidation (Figure 5a–c). TBA, EtOH, and FFA were used to quench ˙OH, SO4˙/˙OH, and 1O2, respectively [21,22]. N2 was bubbled into suspensions to eliminate the interference of dissolved O2 on ACE degradation. With the addition of TBA, EtOH, or FFA into the reaction system at pH 3 (Figure 5a), respectively, the removal of ACE was completely inhibited, which indicated that ˙OH and 1O2 were majorly responsible for ACE degradation. A slight decrease in the removal efficiency for ACE was observed in cubic Cu2O/PMS system after bubbling N2, meaning that dissolved O2 might not participate in oxidation reactions at pH 3. Under pH 5, the degradation efficiencies of ACE were 90.65, 90.63, and 0% with TBA, EtOH, and FFA as quenching agents (Figure 5b), respectively, which meant that the contribution of 1O2 and SO4˙/˙OH toward ACE removal were 90.63 and 9.37%. Figure 5b showed that ACE degradation was obviously suppressed in N2 atmosphere with the removal efficiency of 26.95%. Thus, 1O2 played a vital role during ACE degradation at pH 5 and the action of dissolved O2 was not neglected. In alkaline condition of pH 11, a similar result was obtained (Figure 5c), wherein the addition of TBA displayed no obvious impact on ACE removal, while the degradation efficiency decreased to 81.89% after introducing EtOH, further confirming that 18.11% of ACE was degraded by SO4˙ radicals. Once adding FFA into the catalytic system, the degradation of ACE was entirely suppressed, which demonstrated that 1O2 served as the major ROS during degradation at pH 11 and its contribution toward ACE removal was 81.89%. Additionally, 94% of ACE was eliminated at N2 atmosphere, and the slight inhibition effect was similar to the results obtained from pH 3.

Figure 5 
               (a–c) Effects of different quenchers on ACE degradation in cubic Cu2O/PMS system at (a) pH 3, (b) pH 5, and (c) pH 11. EPR spectra of DMPO-SO4˙−, DMPO-˙OH, and TEMP-1O2 for PMS activation in N2 atmosphere under (d) pH 3, (e) pH 5, and (f) pH 11.
Figure 5

(a–c) Effects of different quenchers on ACE degradation in cubic Cu2O/PMS system at (a) pH 3, (b) pH 5, and (c) pH 11. EPR spectra of DMPO-SO4˙, DMPO-˙OH, and TEMP-1O2 for PMS activation in N2 atmosphere under (d) pH 3, (e) pH 5, and (f) pH 11.

To explore the generation of ROS for ACE degradation in cubic Cu2O/PMS system, spin-trapping EPR spectra were performed at pH 5 in air atmosphere. As observed from Figure S3a, the typical four-line spectra with relative intensities of 1:2:2:1 were detected in different Cu2O/PMS systems by using DMPO as trapping agent, demonstrating that DMPO-˙OH adducts were identified with hyperfine splitting constant of α N = α H = 14.9 G1112 [23]. And also, DMPO-SO4˙ adducts were found in all these systems, of which six special peaks with hyperfine splitting constants of α N = 13.2 G, α H = 9.6 G, α H = 1.48 G, and α H = 0.78 G could be identified to originate from SO4˙ radicals [23]. Moreover, three-line spectra of TEMP-1O2 adducts were found in different Cu2O/PMS system (Figure S3b), verifying that 1O2 was produced and oxidized TEMP to TEMPO [24]. On comparing with vertex-truncated and octahedral Cu2O catalysts, the EPR signals from DMPO-˙OH, DMPO-SO4˙, and TEMP-1O2 adducts were significantly enhanced in cubic Cu2O/PMS system, implying that more ˙OH, SO4˙, and 1O2 were generated during PMS activation over cubic Cu2O. Combining with the results from quenching experiments, 1O2 was proved as the dominant ROS for ACE oxidation in Cu2O/PMS system. In order to confirm the generation pathways of 1O2, EPR techniques were also used to explore the changes in ROS in Cu2O/PMS systems at different solution pH in N2 atmosphere. Observing from Figure 5d, no EPR signals of DMPO-SO4˙ adducts were detected, while some ˙OH radicals were captured during ACE degradation at pH 3, which was probably due to Cu(iii) hydrolysis [25]. Interestingly, the elimination of dissolved O2 prevented the generation of O2˙ in this system. And meanwhile, after adding TBA to cubic Cu2O/PMS system to scavenge ˙OH radicals during PMS activation, no EPR signals of TEMP-1O2 adducts were detected (Figure S4). Thus, it could be speculated that the formation of 1O2 was derived from the disproportionation reaction of ˙OH similar to previous report [26]. Under pH 5, only ˙OH and SO4˙ were observed in the suspensions and are responsible for ACE oxidation (Figure 5e). By contrast, no TEMP-1O2 adducts emerged due to lack of O2 source, which indicated the generation of 1O2 from the dissolved O2. In alkaline condition of pH 11, all signals of TEMP-1O2, DMPO-SO4˙, and DMPO-˙OH were monitored (Figure 5f), confirming the generation of SO4˙, ˙OH, and 1O2 through direct activation of PMS by cubic Cu2O. Besides, at pH 11, the ACE degradation showed no obvious change in N2 atmosphere, which suggested that dissolved O2 did not participate in reactions and the generation of 1O2 was derived from the SO5˙ hydrolysis or disproportionation reaction [27]. Overall, the desired cubic Cu2O catalysts not only exhibited superior catalytic performances, but also adapted well to a wide pH range. Note that 1O2 was extremely important to organic pollutants removal in Cu2O/PMS system, and the degradation mechanism verified that the non-radical process was vital for PMS activation by cubic Cu2O.

The confocal Raman was further performed to observe in situ the interaction processes of the cubic Cu2O/PMS system. As displayed in Figure 6a, three peaks at 880, 980, and 1,060 cm−1 could be observed in the fresh PMS solution alone, which belonged to the stretching vibration of O–O bonds in HSO 5 , and symmetrical stretching vibrations from SO4 2− and HSO 5 , respectively [28,29]. Besides, pure ACE exhibited a broad vibration band centering at 780 cm−1, which was also observed in ACE/Cu2O/PMS systems. Surprisingly, after the adsorption of ACE onto the metal sites of cubic Cu2O, two new characteristic peaks appeared at approximately 558 and 1,092 cm−1, which belonged to the Cu–N stretching vibrations and thus confirmed the formation of Cu–ACE complexes [28]. Similarly, the special peaks (Cu–N) also emerged in ACE/Cu2O/PMS suspensions with different solution pH, meaning that ACE could interact well with cubic Cu2O in a wide pH range, which benefited for improving the degradation activity.

Figure 6 
               (a) In situ Raman spectra of ACE, PMS, ACE/Cubic Cu2O, and ACE/Cubic Cu2O/PMS at different solution pH. The XPS spectra of (b) Cu 2p and (c) O 1s for cubic Cu2O before and after degradation reactions. (d) The removal mechanisms in various pH for removing ACE.
Figure 6

(a) In situ Raman spectra of ACE, PMS, ACE/Cubic Cu2O, and ACE/Cubic Cu2O/PMS at different solution pH. The XPS spectra of (b) Cu 2p and (c) O 1s for cubic Cu2O before and after degradation reactions. (d) The removal mechanisms in various pH for removing ACE.

Based on quenching experiments, EPR spectra, and in situ Raman spectra, the possible mechanisms for ACE degradation were proposed. Three alternative formation pathways of ROS under different pH were supposed. (i) For the degradation process in Cu2O/PMS system at pH 3, Cu(i) would react with HSO 5 to produce Cu(iii) (equation (4)), which was further hydrolyzed to acquire ˙OH and H+ ions (equation (5)). It has been reported that Cu(iii) could rapidly convert PMSO into PMSO2 by the oxygen transfer reaction [30]. To validate the formation of Cu(iii) as intermediate products during degradation, PMSO was added into the cubic Cu2O/PMS system. Consequently, the concentration of PMSO was reduced from 1.0 to 0.7 mmol/L, while an obvious increase in PMSO2 concentration (from 0 to 0.3 mmol/L) was observed, which further proved the existence of Cu(iii) during PMS activation. Meanwhile, 1O2 was derived from the disproportionation reaction of ˙OH (equation (6)). At last, 1O2 and ˙OH worked as major active species to attack and destroy ACE molecules to other smaller oxidized products in acid solution. (ii) At pH 5, PMS mainly existed as HSO 5 anions, which could be activated by Cu(i) to yield seldom ˙OH and SO4˙ radicals (equations (7) and (8)) [31]. While, SO4˙ and ˙OH radicals were not the main ROS for ACE removal as mentioned in Figure 5b. Based on the quenching experiments and EPR trapping results, we conjectured that Cu(i) could react with O2 to form Cu(ii) and O2˙ (equation (9)), and then 1O2 originated from O2˙, which was produced by the self-reaction of in situ generated O2˙ (equations (10) and (11)) or reactions of O2˙ with ˙OH (equation (12)). (iii) Under pH 11, dissolved O2 did not participate in the formation of 1O2 during reactions, and the dominant species for PMS in suspensions were SO5 2− anions [32], which might react with HSO 5 to form 1O2 (equation (13)). In addition, SO4˙ from Cu(i)-induced PMS activation would react with OH to generate ˙OH (equation (14)). Meanwhile, Cu(ii) could combine with HSO 5 to generate SO5˙ (equation (15)), which promoted the generation of 1O2 (equations (16) and (17)). Finally, the electron transfer and chemical states of the fresh and used cubic Cu2O after reacting with PMS activation were also investigated by XPS spectra, and the results are displayed in Figure 6b and c. It could be clearly noted that, by contrast to fresh cubic Cu2O, the content of Cu(ii) in the copper species after oxidation degradation increased from 17 to 31%. This could be resulted from the generation process of 1O2, during which Cu(i) was oxidized to high valence copper species (e.g., Cu(ii) and Cu(iii)) after reacting with PMS, and simultaneously, Cu(ii) would also be reduced to Cu(i) through degradation reactions, forming a cyclic reaction [33]. Due to the poisoning of catalyst in actual reactions, Cu(ii) species could not be fully converted into Cu(i) after PMS activation. As for the O 1s spectra in Figure 6c, it could be noted that the ratio of adsorbed oxygen increased from 24% (fresh cubic Cu2O) to 35% (used cubic Cu2O). The phenomenon was probably due to the involvement of the OH in H2O for PMS activation, resulting in the formation of more adsorbed oxygen species on the surface of catalysts. Thus, the XPS analysis provided powerful evidence with the possible mechanisms, which was definitely concluded in Figure 6d.

(4) Cu ( I ) + HSO 5 Cu ( III ) + OH + SO 4 2 ,

(5) Cu ( III ) + H 2 O Cu ( II ) + H + + ˙ OH ,

(6) 4 ˙ OH O 2 1 + 2H 2 O ,

(7) Cu ( I ) + HSO 5 Cu ( II ) + OH + SO 4 ˙ ,

(8) SO 4 ˙ + H 2 O SO 4 2 + ˙ OH + H + ,

(9) Cu ( I ) + O 2 Cu ( II ) + O 2 ˙ ,

(10) 2 O 2 ˙ + 2 H 2 O O 2 1 + 2OH + H 2 O 2 ,

(11) 2 O 2 ˙ + 2H + O 2 1 + H 2 O 2 ,

(12) O 2 ˙ + ˙ OH O 2 1 + OH ,

(13) HSO 5 + SO 5 2 SO 4 2 + HSO 4 + O 2 1 ,

(14) SO 4 ˙ + OH SO 4 2 + ˙ OH ,

(15) Cu ( II ) + HSO 5 Cu ( I ) + H + + SO 5 ˙ ,

(16) 2SO 5 ˙ + H 2 O 2HSO 4 + 1 / 2 O 2 1 ,

(17) SO 5 ˙ + SO 5 ˙ O 2 1 + 2SO 4 2 .

4 Conclusion

In summary, a potential cubic Cu2O catalyst was successfully developed and employed to efficiently activate PMS for the refractory pollutants’ removal. The superior catalytic oxidation behaviors of cubic Cu2O with {100} facets could be ascribed to its rapid electron transfer and strong PMS adsorption ability. Consequently, cubic Cu2O displayed a higher degradation rate for ACE (0.61 min−1) by PMS activation than that of vertex-truncated octahedral Cu2O (0.35 min−1) and octahedral Cu2O (0.23 min−1), and the highly-efficient catalytic activity could be achieved in a wide pH range of 3–11. The mechanistic study confirmed that 1O2 was dominant ROS during oxidation reactions, which was derived from PMS activation and mainly depended on the redox cycle of Cu species in cubic Cu2O. This work shed new light on PMS-AOPs toward Cu-based catalysts, and offered a sustainable strategy for wastewater purification by non-radical reactions.


# These authors contributed equally to this work.


  1. Funding information: This work was financially supported by the National Natural Science Foundation of China (No. 22106047).

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors state no conflict of interest.

References

[1] Cai H, Zou J, Lin J, Li J, Huang Y, Zhang S, et al. Sodium hydroxide-enhanced acetaminophen elimination in heat/peroxymonosulfate system: Production of singlet oxygen and hydroxyl radical. Chem Eng J. 2022;429:132438.10.1016/j.cej.2021.132438Search in Google Scholar

[2] Qutob M, Rafatullah M, Qamar M, Alorfi HS, Al-Romaizan AN, Hussein MA. A review on heterogeneous oxidation of acetaminophen based on micro and nanoparticles catalyzed by different activators. Nanotechnol Rev. 2022;11:497–525.10.1515/ntrev-2022-0030Search in Google Scholar

[3] Xie F, Zhu W, Lin P, Zhang J, Hao Z, Zhang J, et al. A bimetallic (Co/Fe) modified nickel foam (NF) anode as the peroxymonosulfate (PMS) activator: Characteristics and mechanism. Sep Purif Technol. 2022;296:121429.10.1016/j.seppur.2022.121429Search in Google Scholar

[4] Zhang S, Song S, Gu P, Ma R, Wei D, Zhao G, et al. Visible-light-driven activation of persulfate over cyano and hydroxyl group co-modified mesoporous g-C3N4 for boosting bisphenol A degradation. J Mater Chem A. 2019;7:5552–60.10.1039/C9TA00339HSearch in Google Scholar

[5] Qi J, Yang X, Pan PY, Huang T, Yang X, Wang CC, et al. Interface engineering of Co(OH)2 nanosheets growing on the KNbO3 perovskite based on electronic structure modulation for enhanced peroxymonosulfate activation. Environ Sci Technol. 2022;56:5200–12.10.1021/acs.est.1c08806Search in Google Scholar PubMed

[6] Zhang H, Xie C, Chen L, Duan J, Li F, Liu W. Different reaction mechanisms of SO4˙− and ˙OH with organic compound interpreted at molecular orbital level in Co(II)/peroxymonosulfate catalytic activation system. Water Res. 2023;229:119392.10.1016/j.watres.2022.119392Search in Google Scholar PubMed

[7] Wu L, Li B, Li Y, Fan X, Zhang F, Zhang G, et al. Preferential growth of the cobalt (200) facet in Co@N−C for enhanced performance in a Fenton-like reaction. ACS Catal. 2021;11:5532–43.10.1021/acscatal.1c00701Search in Google Scholar

[8] Hou J, He X, Zhang S, Yu J, Feng M, Li X. Recent advances in cobalt-activated sulfate radical-based advanced oxidation processes for water remediation: A review. Sci Total Environ. 2021;770:145311.10.1016/j.scitotenv.2021.145311Search in Google Scholar PubMed

[9] Hao T, Huang Y, Li F, Wu Y, Fang L. Facet-dependent Fe(ii) redox chemistry on iron oxide for organic pollutant transformation and mechanisms. Water Res. 2022;219:118587.10.1016/j.watres.2022.118587Search in Google Scholar PubMed

[10] Zhang DF, Zhang H, Guo L, Zheng K, Han XD, Zhang Z. Delicate control of crystallographic facet-oriented Cu2O nanocrystals and the correlated adsorption ability. J Mater Chem. 2009;19:5220–5.10.1039/b816349aSearch in Google Scholar

[11] Hafner J. Ab-initio simulations of materials using VASP: Density-functional theory and beyond. J Comput Chem. 2008;29:2044–78.10.1002/jcc.21057Search in Google Scholar PubMed

[12] Kresse G, Joubert D. From ultrasoft pseudopotentials to the projector augmented-wave method. Phys Rev B. 1999;59:1758–75.10.1103/PhysRevB.59.1758Search in Google Scholar

[13] Perdew JP, Burke K, Ernzerhof M. Generalized gradient approximation made simple. Phys Rev Lett. 1996;77:3865–8.10.1103/PhysRevLett.77.3865Search in Google Scholar PubMed

[14] Ropo M, Kokko K, Vitos L. Assessing the perdew-burke-ernzerhof exchange-correlation density functional revised for metallic bulk and surface systems. Phys Rev B. 2008;77:195445.10.1103/PhysRevB.77.195445Search in Google Scholar

[15] Grimme S. Supramolecular binding thermodynamics by dispersion-corrected density functional theory. Chem Eur J. 2012;18:9955–64.10.1002/chem.201200497Search in Google Scholar PubMed

[16] Liu X, Xu M, Zhang X, Wang W, Feng X, Song A. Pulsed-laser-deposited, single-crystalline Cu2O films with low resistivity achieved through manipulating the oxygen pressure. Appl Surf Sci. 2018;435:305–11.10.1016/j.apsusc.2017.11.119Search in Google Scholar

[17] Zhang S, Liu Y, Ma R, Jia D, Wen T, Ai Y, et al. Molybdenum (VI)-oxo clusters incorporation activates g-C3N4 with simultaneously regulating charge transfer and reaction centers for boosting photocatalytic performance. Adv Funct Mater. 2022;32:2204175.10.1002/adfm.202204175Search in Google Scholar

[18] Liu W, Shi M, Li Y, Wu Z, Yang L, Zhang S, et al. Congregated-electrons-strengthened anchoring and mineralization of gaseous formaldehyde on a novel self-supporting Cu2-xSe/Cu2O heterojunction photocatalyst under visible lights: A viable mesh for designing air purifier. Appl Catal B. 2022;312:121427.10.1016/j.apcatb.2022.121427Search in Google Scholar

[19] He X, O’Shea KE. Selective oxidation of H1-antihistamines by unactivated peroxymonosulfate (PMS): Influence of inorganic anions and organic compounds. Water Res. 2020;186:116401.10.1016/j.watres.2020.116401Search in Google Scholar PubMed

[20] Song Y, Li X, Li C, Li J, Dong Z, Zhang M, et al. Exploring and comparing the roles of Ca2+ and Mg2+ in small-sized natural organics-induced charged nanofiltration membrane fouling. Sep Purif Technol. 2020;251:117415.10.1016/j.seppur.2020.117415Search in Google Scholar

[21] Li J, Zhu W, Gao Y, Lin P, Liu J, Zhang J, et al. The catalyst derived from the sulfurized Co-doped metal–organic framework (MOF) for peroxymonosulfate (PMS) activation and its application to pollutant removal. Sep Purif Technol. 2022;285:120362.10.1016/j.seppur.2021.120362Search in Google Scholar

[22] Zhang S, Liu Y, Gu P, Ma R, Wen T, Zhao G, et al. Enhanced photodegradation of toxic organic pollutants using dual-oxygendoped porous g-C3N4: Mechanism exploration from both experimental and DFT studies. Appl Catal B. 2019;248:1–10.10.1016/j.apcatb.2019.02.008Search in Google Scholar

[23] Zhou Z, Huang J, Zeng G, Yang R, Xu Z, Zhou Z, et al. Insights into the removal of organic contaminants by calcium sulfite activation with Fe(iii): Performance, kinetics, and mechanisms. Water Res. 2022;221:118792.10.1016/j.watres.2022.118792Search in Google Scholar PubMed

[24] Zheng W, Chen Y, Fu H, Yan Z, Lei Z, Duan W, et al. Reactive species conversion into 1O2 promotes substantial inhibition of chlorinated byproduct formation during electrooxidation of phenols in Cl−-laden wastewater. Water Res. 2022;225:119143.10.1016/j.watres.2022.119143Search in Google Scholar PubMed

[25] Wang Y, Wu Y, Yu Y, Pan T, Li D, Lambropoulou D, et al. Natural polyphenols enhanced the Cu(ii)/peroxymonosulfate (PMS) oxidation: The contribution of Cu(iii) and HO˙. Water Res. 2020;186:116326.10.1016/j.watres.2020.116326Search in Google Scholar PubMed

[26] Yi Q, Ji J, Shen B, Dong C, Liu J, Zhang J, et al. Singlet oxygen triggered by superoxide radicals in a molybdenum cocatalytic fenton reaction with enhanced REDOX activity in the environment. Environ Sci Technol. 2019;53:9725–33.10.1021/acs.est.9b01676Search in Google Scholar PubMed

[27] Yao Y, Wang C, Yan X, Zhang H, Xiao C, Qi J, et al. Rational regulation of Co−N−C coordination for high-efficiency generation of 1O2 toward nearly 100% selective degradation of organic pollutants. Environ Sci Technol. 2022;56:8833–43.10.1021/acs.est.2c00706Search in Google Scholar PubMed

[28] Mi X, Zhong H, Zhang H, Xu S, Li Y, Wang H, et al. Trace cupric species triggered decomposition of peroxymonosulfate and degradation of organic pollutants: Cu(iii) being the primary and selective intermediate oxidant. Environ Sci Technol. 2022;56:2637–46.10.1021/acs.est.1c06762Search in Google Scholar PubMed

[29] Wang L, Xu H, Jiang N, Wang Z, Jiang J, Zhang T. Facilitating redox cycles of copper species by pollutants in peroxymonosulfate activation. Environ Sci Technol. 2020;54:4686–94.10.1021/acs.est.0c00284Search in Google Scholar PubMed

[30] Chen N, Lee D, Kim MS, Shang H, Cao S, Park EJ, et al. Activation of molecular oxygen by tenorite and ascorbic acid: Generation of high-valent copper species for organic compound oxidation. J Hazard Mater. 2022;440:129839.10.1016/j.jhazmat.2022.129839Search in Google Scholar

[31] Oh W, Dong Z, Lim T. Generation of sulfate radical through heterogeneous catalysis for organic contaminants removal: Current development, challenges and prospects. Appl Catal B. 2016;194:169–201.10.1016/j.apcatb.2016.04.003Search in Google Scholar

[32] Qi J, Liu J, Sun F, Huang T, Duan J, Liu W. High active amorphous Co(OH)2 nanocages as peroxymonosulfate activator for boosting acetaminophen degradation and DFT calculation. Chinese Chem Lett. 2021;32:1814–8.10.1016/j.cclet.2020.11.026Search in Google Scholar

[33] Ding Y, Li D, Zuo S, Guan Z, Ding S. Boron-doping accelerated Cu(ii)/Cu(i) cycle for enhancing peroxymonosulfate activation. Sep Purif Technol. 2022;282:120086.10.1016/j.seppur.2021.120086Search in Google Scholar

Received: 2022-12-25
Revised: 2023-03-15
Accepted: 2023-04-01
Published Online: 2023-06-14

© 2023 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Research Articles
  2. Preparation of CdS–Ag2S nanocomposites by ultrasound-assisted UV photolysis treatment and its visible light photocatalysis activity
  3. Significance of nanoparticle radius and inter-particle spacing toward the radiative water-based alumina nanofluid flow over a rotating disk
  4. Aptamer-based detection of serotonin based on the rapid in situ synthesis of colorimetric gold nanoparticles
  5. Investigation of the nucleation and growth behavior of Ti2AlC and Ti3AlC nano-precipitates in TiAl alloys
  6. Dynamic recrystallization behavior and nucleation mechanism of dual-scale SiCp/A356 composites processed by P/M method
  7. High mechanical performance of 3-aminopropyl triethoxy silane/epoxy cured in a sandwich construction of 3D carbon felts foam and woven basalt fibers
  8. Applying solution of spray polyurea elastomer in asphalt binder: Feasibility analysis and DSR study based on the MSCR and LAS tests
  9. Study on the chronic toxicity and carcinogenicity of iron-based bioabsorbable stents
  10. Influence of microalloying with B on the microstructure and properties of brazed joints with Ag–Cu–Zn–Sn filler metal
  11. Thermohydraulic performance of thermal system integrated with twisted turbulator inserts using ternary hybrid nanofluids
  12. Study of mechanical properties of epoxy/graphene and epoxy/halloysite nanocomposites
  13. Effects of CaO addition on the CuW composite containing micro- and nano-sized tungsten particles synthesized via aluminothermic coupling with silicothermic reduction
  14. Cu and Al2O3-based hybrid nanofluid flow through a porous cavity
  15. Design of functional vancomycin-embedded bio-derived extracellular matrix hydrogels for repairing infectious bone defects
  16. Study on nanocrystalline coating prepared by electro-spraying 316L metal wire and its corrosion performance
  17. Axial compression performance of CFST columns reinforced by ultra-high-performance nano-concrete under long-term loading
  18. Tungsten trioxide nanocomposite for conventional soliton and noise-like pulse generation in anomalous dispersion laser cavity
  19. Microstructure and electrical contact behavior of the nano-yttria-modified Cu-Al2O3/30Mo/3SiC composite
  20. Melting rheology in thermally stratified graphene-mineral oil reservoir (third-grade nanofluid) with slip condition
  21. Re-examination of nonlinear vibration and nonlinear bending of porous sandwich cylindrical panels reinforced by graphene platelets
  22. Parametric simulation of hybrid nanofluid flow consisting of cobalt ferrite nanoparticles with second-order slip and variable viscosity over an extending surface
  23. Chitosan-capped silver nanoparticles with potent and selective intrinsic activity against the breast cancer cells
  24. Multi-core/shell SiO2@Al2O3 nanostructures deposited on Ti3AlC2 to enhance high-temperature stability and microwave absorption properties
  25. Solution-processed Bi2S3/BiVO4/TiO2 ternary heterojunction photoanode with enhanced photoelectrochemical performance
  26. Electroporation effect of ZnO nanoarrays under low voltage for water disinfection
  27. NIR-II window absorbing graphene oxide-coated gold nanorods and graphene quantum dot-coupled gold nanorods for photothermal cancer therapy
  28. Nonlinear three-dimensional stability characteristics of geometrically imperfect nanoshells under axial compression and surface residual stress
  29. Investigation of different nanoparticles properties on the thermal conductivity and viscosity of nanofluids by molecular dynamics simulation
  30. Optimized Cu2O-{100} facet for generation of different reactive oxidative species via peroxymonosulfate activation at specific pH values to efficient acetaminophen removal
  31. Brownian and thermal diffusivity impact due to the Maxwell nanofluid (graphene/engine oil) flow with motile microorganisms and Joule heating
  32. Appraising the dielectric properties and the effectiveness of electromagnetic shielding of graphene reinforced silicone rubber nanocomposite
  33. Synthesis of Ag and Cu nanoparticles by plasma discharge in inorganic salt solutions
  34. Low-cost and large-scale preparation of ultrafine TiO2@C hybrids for high-performance degradation of methyl orange and formaldehyde under visible light
  35. Utilization of waste glass with natural pozzolan in the production of self-glazed glass-ceramic materials
  36. Mechanical performance of date palm fiber-reinforced concrete modified with nano-activated carbon
  37. Melting point of dried gold nanoparticles prepared with ultrasonic spray pyrolysis and lyophilisation
  38. Graphene nanofibers: A modern approach towards tailored gypsum composites
  39. Role of localized magnetic field in vortex generation in tri-hybrid nanofluid flow: A numerical approach
  40. Intelligent computing for the double-diffusive peristaltic rheology of magneto couple stress nanomaterials
  41. Bioconvection transport of upper convected Maxwell nanoliquid with gyrotactic microorganism, nonlinear thermal radiation, and chemical reaction
  42. 3D printing of porous Ti6Al4V bone tissue engineering scaffold and surface anodization preparation of nanotubes to enhance its biological property
  43. Bioinspired ferromagnetic CoFe2O4 nanoparticles: Potential pharmaceutical and medical applications
  44. Significance of gyrotactic microorganisms on the MHD tangent hyperbolic nanofluid flow across an elastic slender surface: Numerical analysis
  45. Performance of polycarboxylate superplasticisers in seawater-blended cement: Effect from chemical structure and nano modification
  46. Entropy minimization of GO–Ag/KO cross-hybrid nanofluid over a convectively heated surface
  47. Oxygen plasma assisted room temperature bonding for manufacturing SU-8 polymer micro/nanoscale nozzle
  48. Performance and mechanism of CO2 reduction by DBD-coupled mesoporous SiO2
  49. Polyarylene ether nitrile dielectric films modified by HNTs@PDA hybrids for high-temperature resistant organic electronics field
  50. Exploration of generalized two-phase free convection magnetohydrodynamic flow of dusty tetra-hybrid Casson nanofluid between parallel microplates
  51. Hygrothermal bending analysis of sandwich nanoplates with FG porous core and piezomagnetic faces via nonlocal strain gradient theory
  52. Design and optimization of a TiO2/RGO-supported epoxy multilayer microwave absorber by the modified local best particle swarm optimization algorithm
  53. Mechanical properties and frost resistance of recycled brick aggregate concrete modified by nano-SiO2
  54. Self-template synthesis of hollow flower-like NiCo2O4 nanoparticles as an efficient bifunctional catalyst for oxygen reduction and oxygen evolution in alkaline media
  55. High-performance wearable flexible strain sensors based on an AgNWs/rGO/TPU electrospun nanofiber film for monitoring human activities
  56. High-performance lithium–selenium batteries enabled by nitrogen-doped porous carbon from peanut meal
  57. Investigating effects of Lorentz forces and convective heating on ternary hybrid nanofluid flow over a curved surface using homotopy analysis method
  58. Exploring the potential of biogenic magnesium oxide nanoparticles for cytotoxicity: In vitro and in silico studies on HCT116 and HT29 cells and DPPH radical scavenging
  59. Enhanced visible-light-driven photocatalytic degradation of azo dyes by heteroatom-doped nickel tungstate nanoparticles
  60. A facile method to synthesize nZVI-doped polypyrrole-based carbon nanotube for Ag(i) removal
  61. Improved osseointegration of dental titanium implants by TiO2 nanotube arrays with self-assembled recombinant IGF-1 in type 2 diabetes mellitus rat model
  62. Functionalized SWCNTs@Ag–TiO2 nanocomposites induce ROS-mediated apoptosis and autophagy in liver cancer cells
  63. Triboelectric nanogenerator based on a water droplet spring with a concave spherical surface for harvesting wave energy and detecting pressure
  64. A mathematical approach for modeling the blood flow containing nanoparticles by employing the Buongiorno’s model
  65. Molecular dynamics study on dynamic interlayer friction of graphene and its strain effect
  66. Induction of apoptosis and autophagy via regulation of AKT and JNK mitogen-activated protein kinase pathways in breast cancer cell lines exposed to gold nanoparticles loaded with TNF-α and combined with doxorubicin
  67. Effect of PVA fibers on durability of nano-SiO2-reinforced cement-based composites subjected to wet-thermal and chloride salt-coupled environment
  68. Effect of polyvinyl alcohol fibers on mechanical properties of nano-SiO2-reinforced geopolymer composites under a complex environment
  69. In vitro studies of titanium dioxide nanoparticles modified with glutathione as a potential drug delivery system
  70. Comparative investigations of Ag/H2O nanofluid and Ag-CuO/H2O hybrid nanofluid with Darcy-Forchheimer flow over a curved surface
  71. Study on deformation characteristics of multi-pass continuous drawing of micro copper wire based on crystal plasticity finite element method
  72. Properties of ultra-high-performance self-compacting fiber-reinforced concrete modified with nanomaterials
  73. Prediction of lap shear strength of GNP and TiO2/epoxy nanocomposite adhesives
  74. A novel exploration of how localized magnetic field affects vortex generation of trihybrid nanofluids
  75. Fabrication and physicochemical characterization of copper oxide–pyrrhotite nanocomposites for the cytotoxic effects on HepG2 cells and the mechanism
  76. Thermal radiative flow of cross nanofluid due to a stretched cylinder containing microorganisms
  77. In vitro study of the biphasic calcium phosphate/chitosan hybrid biomaterial scaffold fabricated via solvent casting and evaporation technique for bone regeneration
  78. Insights into the thermal characteristics and dynamics of stagnant blood conveying titanium oxide, alumina, and silver nanoparticles subject to Lorentz force and internal heating over a curved surface
  79. Effects of nano-SiO2 additives on carbon fiber-reinforced fly ash–slag geopolymer composites performance: Workability, mechanical properties, and microstructure
  80. Energy bandgap and thermal characteristics of non-Darcian MHD rotating hybridity nanofluid thin film flow: Nanotechnology application
  81. Green synthesis and characterization of ginger-extract-based oxali-palladium nanoparticles for colorectal cancer: Downregulation of REG4 and apoptosis induction
  82. Abnormal evolution of resistivity and microstructure of annealed Ag nanoparticles/Ag–Mo films
  83. Preparation of water-based dextran-coated Fe3O4 magnetic fluid for magnetic hyperthermia
  84. Statistical investigations and morphological aspects of cross-rheological material suspended in transportation of alumina, silica, titanium, and ethylene glycol via the Galerkin algorithm
  85. Effect of CNT film interleaves on the flexural properties and strength after impact of CFRP composites
  86. Self-assembled nanoscale entities: Preparative process optimization, payload release, and enhanced bioavailability of thymoquinone natural product
  87. Structure–mechanical property relationships of 3D-printed porous polydimethylsiloxane films
  88. Nonlinear thermal radiation and the slip effect on a 3D bioconvection flow of the Casson nanofluid in a rotating frame via a homotopy analysis mechanism
  89. Residual mechanical properties of concrete incorporated with nano supplementary cementitious materials exposed to elevated temperature
  90. Time-independent three-dimensional flow of a water-based hybrid nanofluid past a Riga plate with slips and convective conditions: A homotopic solution
  91. Lightweight and high-strength polyarylene ether nitrile-based composites for efficient electromagnetic interference shielding
  92. Review Articles
  93. Recycling waste sources into nanocomposites of graphene materials: Overview from an energy-focused perspective
  94. Hybrid nanofiller reinforcement in thermoset and biothermoset applications: A review
  95. Current state-of-the-art review of nanotechnology-based therapeutics for viral pandemics: Special attention to COVID-19
  96. Solid lipid nanoparticles for targeted natural and synthetic drugs delivery in high-incidence cancers, and other diseases: Roles of preparation methods, lipid composition, transitional stability, and release profiles in nanocarriers’ development
  97. Critical review on experimental and theoretical studies of elastic properties of wurtzite-structured ZnO nanowires
  98. Polyurea micro-/nano-capsule applications in construction industry: A review
  99. A comprehensive review and clinical guide to molecular and serological diagnostic tests and future development: In vitro diagnostic testing for COVID-19
  100. Recent advances in electrocatalytic oxidation of 5-hydroxymethylfurfural to 2,5-furandicarboxylic acid: Mechanism, catalyst, coupling system
  101. Research progress and prospect of silica-based polymer nanofluids in enhanced oil recovery
  102. Review of the pharmacokinetics of nanodrugs
  103. Engineered nanoflowers, nanotrees, nanostars, nanodendrites, and nanoleaves for biomedical applications
  104. Research progress of biopolymers combined with stem cells in the repair of intrauterine adhesions
  105. Progress in FEM modeling on mechanical and electromechanical properties of carbon nanotube cement-based composites
  106. Antifouling induced by surface wettability of poly(dimethyl siloxane) and its nanocomposites
  107. TiO2 aerogel composite high-efficiency photocatalysts for environmental treatment and hydrogen energy production
  108. Structural properties of alumina surfaces and their roles in the synthesis of environmentally persistent free radicals (EPFRs)
  109. Nanoparticles for the potential treatment of Alzheimer’s disease: A physiopathological approach
  110. Current status of synthesis and consolidation strategies for thermo-resistant nanoalloys and their general applications
  111. Recent research progress on the stimuli-responsive smart membrane: A review
  112. Dispersion of carbon nanotubes in aqueous cementitious materials: A review
  113. Applications of DNA tetrahedron nanostructure in cancer diagnosis and anticancer drugs delivery
  114. Magnetic nanoparticles in 3D-printed scaffolds for biomedical applications
  115. An overview of the synthesis of silicon carbide–boron carbide composite powders
  116. Organolead halide perovskites: Synthetic routes, structural features, and their potential in the development of photovoltaic
  117. Recent advancements in nanotechnology application on wood and bamboo materials: A review
  118. Application of aptamer-functionalized nanomaterials in molecular imaging of tumors
  119. Recent progress on corrosion mechanisms of graphene-reinforced metal matrix composites
  120. Research progress on preparation, modification, and application of phenolic aerogel
  121. Application of nanomaterials in early diagnosis of cancer
  122. Plant mediated-green synthesis of zinc oxide nanoparticles: An insight into biomedical applications
  123. Recent developments in terahertz quantum cascade lasers for practical applications
  124. Recent progress in dielectric/metal/dielectric electrodes for foldable light-emitting devices
  125. Nanocoatings for ballistic applications: A review
  126. A mini-review on MoS2 membrane for water desalination: Recent development and challenges
  127. Recent updates in nanotechnological advances for wound healing: A narrative review
  128. Recent advances in DNA nanomaterials for cancer diagnosis and treatment
  129. Electrochemical micro- and nanobiosensors for in vivo reactive oxygen/nitrogen species measurement in the brain
  130. Advances in organic–inorganic nanocomposites for cancer imaging and therapy
  131. Advancements in aluminum matrix composites reinforced with carbides and graphene: A comprehensive review
  132. Modification effects of nanosilica on asphalt binders: A review
  133. Decellularized extracellular matrix as a promising biomaterial for musculoskeletal tissue regeneration
  134. Review of the sol–gel method in preparing nano TiO2 for advanced oxidation process
  135. Micro/nano manufacturing aircraft surface with anti-icing and deicing performances: An overview
  136. Cell type-targeting nanoparticles in treating central nervous system diseases: Challenges and hopes
  137. An overview of hydrogen production from Al-based materials
  138. A review of application, modification, and prospect of melamine foam
  139. A review of the performance of fibre-reinforced composite laminates with carbon nanotubes
  140. Research on AFM tip-related nanofabrication of two-dimensional materials
  141. Advances in phase change building materials: An overview
  142. Development of graphene and graphene quantum dots toward biomedical engineering applications: A review
  143. Nanoremediation approaches for the mitigation of heavy metal contamination in vegetables: An overview
  144. Photodynamic therapy empowered by nanotechnology for oral and dental science: Progress and perspectives
  145. Biosynthesis of metal nanoparticles: Bioreduction and biomineralization
  146. Current diagnostic and therapeutic approaches for severe acute respiratory syndrome coronavirus-2 (SARS-COV-2) and the role of nanomaterial-based theragnosis in combating the pandemic
  147. Application of two-dimensional black phosphorus material in wound healing
  148. Special Issue on Advanced Nanomaterials and Composites for Energy Conversion and Storage - Part I
  149. Helical fluorinated carbon nanotubes/iron(iii) fluoride hybrid with multilevel transportation channels and rich active sites for lithium/fluorinated carbon primary battery
  150. The progress of cathode materials in aqueous zinc-ion batteries
  151. Special Issue on Advanced Nanomaterials for Carbon Capture, Environment and Utilization for Energy Sustainability - Part I
  152. Effect of polypropylene fiber and nano-silica on the compressive strength and frost resistance of recycled brick aggregate concrete
  153. Mechanochemical design of nanomaterials for catalytic applications with a benign-by-design focus
Downloaded on 11.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/ntrev-2022-0542/html
Scroll to top button