Panuwat
Lawtae
,
Sutaporn
Meephon
,
Vipada
Dokmai
,
Rungthiwa
Methaapanon
* and
Varong
Pavarajarn
*
Center of Excellence in Particle and Materials Processing Technology, Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, Thailand. E-mail: varong.p@chula.ac.th; rungthiwa.m@chula.ac.th
First published on 27th March 2025
This study provides direct experimental evidence of facet- and pH-dependent interactions governing the adsorption and photocatalytic degradation of diuron, a persistent herbicide, on zinc oxide (ZnO) surfaces. Unlike conventional studies that assume uniform catalyst surfaces, this work systematically measured the interaction strength on different ZnO facets, using atomic force microscopy (AFM)-based force spectroscopy under conditions replicating the reaction environment. Interaction strengths among ZnO surfaces followed the order: O-terminated > Zn-terminated > mixed-terminated. The finding that ZnO powder, with polar Zn- and O-terminated surfaces, exhibited adsorption capacity approximately five times higher than that of ZnO nanorods, which have non-polar mixed-terminated surfaces, despite having an order of magnitude lower surface area further highlights the role of surface interactions in governing adsorption and subsequent photocatalytic performance. Stronger adsorption under acidic conditions enhanced the degradation efficiency, while alkaline conditions altered adsorption orientations and reduced the capacity. The degradation pathways were found to be highly facet- and pH-dependent, leading to distinct sets of intermediates with varying toxicity. Cytogenotoxicity assays revealed that certain degradation products formed under alkaline conditions were more harmful than diuron itself, underscoring the need for optimized photocatalyst designs. This work provides critical insights into facet-dependent interactions and pH effects, paving the way for more effective and safer photocatalytic solutions for environmental remediation.
This critical gap is the main focus of this study. The facet-dependent adsorption and subsequent impact on the photocatalytic degradation of diuron [3-(3,4-dichlorophenyl)-1,1-dimethyl urea], which is a persistent and toxic herbicide widely used in agriculture, on zinc oxide (ZnO) is investigated. ZnO is particularly well-suited for this study as a model system for facet-dependent photocatalysis due to its ability to expose and control various crystallographic facets, including polar (Zn- and O-terminated) and non-polar surfaces, enabling precise investigation of facet-dependent phenomena.7 Compared to other widely studied photocatalysts such as TiO2, ZnO offers several advantages, including enhanced charge carrier mobility,8 tunable surface defects (i.e., oxygen vacancies and Zn interstitials), and greater pH-dependent surface charge variability,9 which directly influence the adsorption and photocatalytic performance. The choice of diuron for this study is particularly relevant because its degradation reactions could generate intermediates with different levels of toxicity, some of which can be more harmful than the parent compound,10 underlining the criticality of using catalysts with controlled facets.
Two forms of ZnO are used, namely ZnO powder (with (0001) zinc-terminated and (000
) oxygen-terminated as dominating surfaces) and ZnO nanorods (exposing (10
0) mixed-terminated non-polar surfaces). Previous studies have shown that the surface reactivity of ZnO is facet-dependent, with enhanced adsorption of oxygen-containing species, e.g., OH−, O2, and O2−, on polar surfaces due to the presence of oxygen vacancies.11 Nevertheless, most studies, including our previous work, are either based on inference without direct measurement of the interaction or on the measurement in air, in which the effect of pH could not be included. In this work, atomic force microscopy (AFM) force spectroscopy is performed in aqueous solutions to directly measure interaction on different ZnO surfaces under replicated experimental conditions. Additionally, due to the amphoteric nature of ZnO, surface properties of which are influenced by pH,12 the interaction strength, the adsorption, as well as the photocatalytic degradation of diuron on different ZnO surfaces in both acidic and alkaline environments are systematically investigated.
Since the specific mechanisms of how surface interactions influence photocatalytic activity are not fully understood, it is usually presumed that effective degradation requires a high surface area, substantial adsorption capacity, and conditions that promote radical generation.13–15 These factors are often prioritized in catalyst design, with little consideration given to the strength and nature of the interaction between the adsorbed molecule and the catalyst surface. In this study, the interaction strength of ZnO surfaces was systematically evaluated using AFM, along with the adsorption and reaction kinetics measurements. These details would provide a deeper mechanistic insight into the facet-dependent surface interactions and how these interactions vary across different pH conditions as well as their subsequent effects on photocatalytic degradation pathways. The findings suggested that the interaction intensity between adsorbed molecules and specific facets could be more essential to reaction activity than the density of active sites on the surface. The unique interactions on different surfaces of the same catalyst materials also resulted in distinct reaction pathways and various by-products with varying degrees of toxicity. The study underlines the importance of selective facets in catalysis and provides a deeper understanding of heterogeneous photocatalytic degradation.
After particle positions on the substrate were identified, the probe was switched to a silicon tip (ContAl, Budget Sensors, Innovative Solutions Bulgaria Limited, Sofia, Bulgaria), whose surface would be consistently negatively charged at all pH levels relevant to this study. The AFM probes were calibrated in water over a glass substrate at room temperature using thermal tuning to determine cantilever spring constants. Contact mode imaging was then used to locate the ZnO surface at the predetermined particle positions.
Force curves (force vs. cantilever displacement) were obtained by recording cantilever deflection as the sample surface was moved toward (approach curve) or retracted (retract curve) from the tip. Zero force was defined as the force when the tip and sample were sufficiently separated, with no cantilever deflection being detected. For robust statistical validation, 50 to 70 force curves were collected from various areas/particles on each ZnO particle surface. For ZnO powder, identification of Zn-terminated and O-terminated surfaces was done by comparing the obtained force with those from standard Zn-terminated and standard O-terminated surfaces of a single crystal ZnO wafer (Semiconductor Wafer Inc.).
Adsorption parameters were determined through non-linear regression using OriginPro 2018 (OriginLab, Northampton, MA, USA). The error function was defined to evaluate the isotherm fit to the experimental equilibrium data, with the regression coefficient (R2) and chi-squared statistic selected as key metrics. An R2 approaching 1 and a chi-squared value near zero indicated strong model alignment with experimental data.18
In the assembly of the microreactor, a Teflon sheet with a thickness of 250 micrometers was placed between two glass pieces to define the microchannel's thickness. One glass was coated with the catalyst, and the other, a blank glass, was drilled to facilitate the inlet and outlet streams. All microstructures were assembled using a stainless steel housing.19 A schematic diagram of the microreactor is provided in the ESI (Fig. S1).† The photocatalytic degradation was operated continuously within the microreactor. The residence time was varied from 1 to 15 minutes by adjusting the flow rate. The initial solution concentration was maintained at 10 ppm, and the pH was adjusted to 4 and 10 using 0.1 M HCl and 0.1 M NaOH, respectively. A 40 W mercury lamp with a spectrum of 350–410 nm served as the light source, positioned at the center for uniform energy distribution. The outlet stream underwent concentration analysis by HPLC (Shimadzu, Class 10VP with a Luna 5μ C18(2) column), while intermediates were identified by LC-MS/MS (Thermo Finnigan, LCQ Advantage).
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Fig. 1 presents high-resolution XPS spectra of the O 1s peak for both ZnO powder and ZnO nanorods under different pH conditions. Deconvolution of the spectra reveals three peaks: the peak near 530 eV (red line) corresponds to lattice oxygen within ZnO; the peak around 531 eV (purple line) is associated with oxygen vacancies or oxygen-deficient regions, indicating surface alterations by defects; the peak near 532 eV (green line) is attributed to the oxygen in functional groups, particularly hydroxyl groups (OH).21 Although these peak positions align with our previous data without aqueous treatment, their relative intensities vary with pH conditions.
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| Fig. 1 High-resolution XPS O 1s spectra deconvolution of ZnO powder (a1–a3) and ZnO nanorods (b1–b3) under varying pH conditions (pH 4, pH 7, and pH 10). | ||
These variations become more evident when comparing the areas under the curves for oxygen vacancies and hydroxyl groups relative to lattice oxygen, as shown in Table 1. The hydroxyl group content on both ZnO catalysts follows the order: pH 7 > pH 4 > pH 10 > air. (The XPS spectra of ZnO in air were previously published.22) The intensity of the hydroxyl group of ZnO immersed in pH-adjusted solutions is significantly higher than that of ZnO in air, indicating that ZnO in solution is more readily hydrolyzed to form surface hydroxide layers (Zn–OH), leading to notable changes in surface chemistry compared to pristine ZnO.23 The hydroxyl formation is more pronounced at neutral pH. The lower intensity of hydroxyl groups at acidic and alkaline pH is likely due to H+ or OH− ions inhibiting their formation, reflecting amphoteric surface reactions.24
| Sample name | Conditions | Ovac/Olattice | OOH/Olattice |
|---|---|---|---|
| ZnO powder | In air | 0.387 | 0.171 |
| pH 4 | 1.103 | 0.545 | |
| pH 7 | 1.144 | 0.891 | |
| pH 10 | 0.516 | 0.385 | |
| ZnO nanorods | In air | 0.519 | 0.253 |
| pH 4 | 1.588 | 0.607 | |
| pH 7 | 1.962 | 1.060 | |
| pH 10 | 0.432 | 0.297 |
The trend in oxygen vacancies aligns with that of surface hydroxyl groups, suggesting a connection between hydroxyl group formation and increased surface reorganization (Table 1). Nevertheless, XPS results alone are not sufficient for a comprehensive understanding of the interaction between adsorbed molecules and the ZnO surfaces. For direct evaluation, atomic force microscopy (AFM) force spectroscopy was used to examine ZnO interaction strengths on each facet under different pH conditions. Integrating XPS with AFM findings will deepen the understanding of pH effects on ZnO surface interactions.
| Surfaces | Adhesion energy (×10−18 J) | ||
|---|---|---|---|
| pH 4 | pH 7 | pH 9 | |
| a The presented data are based on averaging results obtained from at least 60 force–distance curves for each interaction pair. | |||
| O-Terminated | 52.15 ± 4.44 | 42.67 ± 3.37 | 9.40 ± 2.47 |
| Zn-Terminated | 28.33 ± 4.12 | 20.90 ± 2.84 | 31.05 ± 3.69 |
| Mixed-terminated | 16.46 ± 3.12 | 19.16 ± 3.09 | 23.11 ± 3.36 |
For O-terminated surfaces of ZnO powder, the highest adhesion energy (52.2 × 10−18 J) was observed at pH 4. The magnitude of the adhesion energy indicates a strong polar–polar interaction between the positive charge on O-terminated surfaces and the negatively charged silica tip.17 The positive charge on the O-terminated surfaces could result from proton uptake that compensates for the charge on surface oxygen.26 As the pH increased, adhesion energy continued to decrease and dropped sharply to 9.4 × 10−18 J at pH 9, primarily due to repulsive electrostatic forces between negatively charged surfaces. This trend reflects the weaker attraction at higher pH values, as protonation on the O-terminated surfaces diminishes.
For Zn-terminated surfaces of ZnO powder, the adhesion energy to negatively charged silica tips decreased from 28.3 × 10−18 J at pH 4 to 20.9 × 10−18 J at pH 7 and subsequently increased to 31 × 10−18 J at pH 9. This pattern correlates with XPS results of hydroxyl group intensity on the surface, which follows the order pH 7 > pH 4 > pH 10, suggesting a strong influence of the hydroxyl group on the interaction between Zn-terminated surfaces and the silica tips. The partial positive charges on hydrogen atoms within the hydroxyl groups could enhance electrostatic attraction with a negatively charged AFM tip. However, the increased hydroxyl density would increase the number of negatively charged O atoms that could impede the effective rearrangement of hydrogen atoms, affecting adhesion energy trends on Zn-terminated surfaces (Fig. 2).
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| Fig. 2 Comparison of adhesion energies between the AFM probe and ZnO surfaces under different pH conditions. | ||
In the case of mixed-terminated ZnO nanorods, the adhesion energy was relatively low and changed less dramatically across pH levels compared to both Zn- and O-terminated surfaces of ZnO powder. This observation is consistent with previous findings that nonpolar wurtzite surfaces exhibit stable surfaces and low interaction strength.17 The adhesion energy increased from 16.5 × 10−18 J at pH 4 to 23.1 × 10−18 J at pH 9, with more pronounced increases under alkaline conditions. It should be noted that the interatomic Zn–O distance on the mixed-terminated surface is about 0.2 nm,27 while AFM tips are approximately 10 nm, leading to a distributed interaction across the surface rather than with specific Zn or O atoms. Therefore, unlike the polar Zn- and O-terminated surfaces, the mixed-terminated nanorods show more stable charge distribution and less pronounced pH-dependent variation in adhesion energy.
Fig. 3 illustrates the diuron adsorption isotherms for ZnO samples at different pH levels (4, 7, and 10), with nonlinear regression analysis data summarized in Table 3. The model fits the experimental data well, as indicated by low chi-squared values and high R2 values. ZnO powder shows a higher heterogeneity parameter, nF, than ZnO nanorods, indicating greater surface heterogeneity, likely due to the presence of both O- and Zn-terminated surfaces. Conversely, the mixed-terminated surfaces of ZnO nanorods exhibit a more uniform distribution of adsorption energies. Additionally, nF values for ZnO nanorods decrease below 1 as the pH increases, indicating less favorable adsorption. In contrast, the nF values for ZnO powder remain stable to pH. This consistency may result from balanced interactions on O- and Zn-terminated surfaces, with relatively constant adsorption energy distribution across pH levels. AFM results in Fig. 2 support this stability, showing consistent differences between the adhesion energies of Zn- and O-terminated surfaces across the pH range.
| Sample | pH | Freundlich parameter | R 2 | Chi-squared | |
|---|---|---|---|---|---|
| n F | K F | ||||
| ZnO powder | 4 | 1.11 | 0.149 | 0.9990 | 0.0045 |
| 7 | 1.12 | 0.093 | 0.9959 | 0.0084 | |
| 10 | 1.12 | 0.071 | 0.9980 | 0.0020 | |
| ZnO nanorods | 4 | 1.07 | 0.032 | 0.9988 | 0.0009 |
| 7 | 0.99 | 0.018 | 0.9949 | 0.0025 | |
| 10 | 0.95 | 0.012 | 0.9750 | 0.0112 | |
In Fig. 3, the adsorption isotherms of ZnO powder at low diuron concentrations (0–25 mg L−1) are above those of ZnO nanorods across all pH levels, with a steeper slope and a higher binding capacity parameter, KF (Table 3). This suggests that ZnO powder has a higher binding capacity for diuron despite its smaller surface area (1.4 m2 g−1vs. 17 m2 g−1 for nanorods), indicating that adsorption capacity is more influenced by surface interactions than the surface area alone. These findings align with the suggestion by prior research that the polar ZnO surfaces interact more strongly with adsorbed species compared to non-polar ZnO surfaces.30,31 The direct measurement via AFM also shows higher adhesion energies for ZnO powder than ZnO nanorods across the pH range, implying more favorable surface characteristics for diuron adsorption. The stronger surface interactions enhance the adsorption capacity.
Fig. 3 also illustrates the effect of pH on the diuron adsorption capacity for ZnO samples. Both ZnO powder and nanorods exhibit reduced diuron adsorption at higher pH, aligning with decreases in KF. This indicates more efficient adsorption under acidic conditions. The ZnO powder and nanorods have points of zero charge (PZC) at pH 7.9 and 6.7, respectively, implying that they are positively charged below these pH values and negatively charged above them. This observation challenges the view that the overall electrostatic charge of a particle determines how the adsorption capacity changes with pH,32 as diuron (pKa of 13.5) remains neutral at most environmental pH levels. Instead, the local interaction between functional groups of diuron and the specific surface of ZnO should be considered. Under acidic conditions (pH 4), diuron adsorption onto ZnO is driven primarily by strong polar–polar interactions between its negatively polar regions (e.g., oxygen and chlorine atoms) and the positively charged ZnO surfaces. This is corroborated by AFM results, which show strong polar–polar interactions under acidic conditions. At alkaline pH (pH 10), diuron adsorption is driven by interactions between the negatively charged ZnO surfaces and the locally positively charged regions of diuron, such as the aliphatic methyl group, resulting in weaker binding and lower adsorption capacity.
Overall, ZnO powder shows a higher adsorption capacity than ZnO nanorods across all studied pH levels, despite having an order of magnitude lower surface area, due to stronger interactions with diuron. Additionally, the pH markedly influences the nature of these surface interactions, affecting diuron adsorption behavior in distinct ways.
As noted previously, surface interactions at different pH levels significantly influenced diuron adsorption characteristics on ZnO surfaces, which include the adsorption capacity and adsorption orientation, and this adsorption behavior appears to influence how diuron interacts with the radicals formed on the surfaces to form degradation intermediates. The following sections explore its impact on diuron degradation kinetics and the associated reaction pathways.
| Sample | pH | k (min−1) | R 2 | Chi-squared |
|---|---|---|---|---|
| Powder | 4 | 0.173 | 0.950 | 0.122 |
| 7 | 0.153 | 0.953 | 0.091 | |
| 10 | 0.133 | 0.920 | 0.118 | |
| Nanorods | 4 | 0.183 | 0.941 | 0.121 |
| 7 | 0.154 | 0.947 | 0.082 | |
| 10 | 0.119 | 0.954 | 0.064 |
Interestingly, despite enhanced OH production under alkaline conditions, diuron degradation does not increase with pH, indicating that hydroxyl radical availability is not rate-limiting and is already adequate in this system. Consistently, the degradation rate dependency on the diuron concentration, according to the pseudo-first-order kinetics model, suggests that photocatalytic efficiency in this system is primarily driven by adsorption characteristics rather than the availability of radicals. Despite ZnO nanorods having a larger surface area than ZnO powder, the degradation rates of diuron between the two catalysts exhibit no significant differences. This finding supports the literature, indicating that photocatalytic performance is not exclusively dictated by the surface area.42 Instead, the primary driver of diuron degradation is the interaction between ZnO surfaces and diuron molecules. Under acidic conditions, stronger interactions enhance diuron adsorption, bringing molecules closer to the surface and increasing the likelihood of degradation. These results highlight the critical role of surface interactions in photocatalytic activity.
Facet-dependent pathways for the photocatalytic degradation of diuron on ZnO at neutral pH were introduced in our previous work.16 In this work, the influence of various pH was studied. LC-MS/MS analysis of diuron photocatalytic degradation intermediates on ZnO samples at pH 4 is shown in Fig. 5. The majority of intermediates detected under acidic conditions were not formed at neutral pH, confirming that substantial change in diuron/ZnO surface interactions due to pH change drastically affects diuron degradation. In the initial stage, the hydroxyl radicals attack both the aliphatic and aromatic regions of diuron on both ZnO catalysts, indicating that diuron adsorbs on the ZnO surface in a manner that makes both regions accessible. This accessibility aligns with the strong interactions between the negatively charged regions of diuron (e.g., chlorine on the aromatic ring and oxygen on the aliphatic side) and the positively charged ZnO surfaces, as indicated by AFM results. Under acidic conditions, the order of interaction strength among ZnO surfaces is ranked as follows: O-terminated, Zn-terminated, and mixed-terminated surfaces, respectively. These interactions likely enhance diuron's accessibility, facilitating hydroxyl radical attack across the molecule.
At pH 10, the degradation pattern changes almost completely, especially for the degradation on ZnO powder. The pH affects polar surfaces more strongly, as witnessed by AFM results, consequently altering the adsorption posture of the diuron. For ZnO nanorods, radicals initially attack only the aliphatic side of the diuron, while on ZnO powder, both aliphatic and aromatic regions are targeted (Fig. 6). On ZnO powder, negatively charged hydroxide ions predominantly adsorb onto Zn-terminated surfaces, attracting the positively charged methyl groups from the aliphatic side. In contrast, diuron's aromatic region likely interacts with O-terminated surfaces on ZnO powder, which electrostatically repels the oxygen and chlorine atoms. The interaction potentially causes a reorientation of hydrogen atoms of the methyl group and the aromatic ring toward the surface and enables hydroxyl attack on both sides. The formation of identical intermediates (C3 and C18) from the aliphatic regions on both ZnO samples suggests similar adsorption characteristics on Zn-terminated surfaces of ZnO powder and mixed-terminated surfaces of ZnO nanorods.
These findings highlight the role of ZnO surface interactions in shaping the degradation pathway and specific products of diuron.
In contrast, under alkaline conditions (pH 10), O-terminated surfaces become electron-rich, creating repulsive electrostatic forces against the chlorine and oxygen atoms of diuron. This repulsion could lead to the reorientation of the diuron's positively charged hydrogen atoms toward the surface (refer to Fig. 7b). Meanwhile, hydroxide ions on the Zn-terminated surfaces create a negative environment that repels the aromatic end of diuron, leaving only the methyl group hydrogens to adsorb onto the surface through weak van der Waals interactions (Fig. 7d). This disordered adsorption configuration under alkaline conditions reduces the accessible adsorption sites, as reflected in the binding capacity (KF), which decreases by approximately 37% at pH 7 and 52% at pH 10 compared to that at pH 4.
For ZnO nanorods (Fig. 7e and f), the adsorption behavior mirrors that of ZnO powder, with lower adsorption capacity at higher pH levels. Diuron adsorption on the mixed-terminated surfaces of ZnO nanorods under acidic conditions (Fig. 7e) is comparable to that on O- and Zn-terminated surfaces under alkaline conditions (Fig. 7f) but shows lower capacity across pH levels. This reduced capacity is attributed to the reduced polarity and attractiveness of mixed-terminated surfaces.
This work employs cytogenotoxicity, indicated by MI and ADR values calculated using eqn (1) and (2), respectively, to represent the toxicity of diuron. Large MI refers to flourishing cell division, indicating low toxicity. On the other hand, high ADR reflects abnormalities in various phases of cell mitosis, hence high toxicity. Low MI and high ADR from diuron solution, compared to the values from deionized water (see Table 5), underline the inherent cytogenotoxicity of diuron. It is also observed that both acidity and basicity also introduce chromosomal irregularities to the cells. Cytogenotoxicity testing was selected among various toxicity assessments due to its relevance to the cellular toxification process in plant cells induced by herbicides such as diuron. It evaluates chromosomal integrity and mitotic activity, serving as an early indicator of genotoxic effects. The cytogenotoxicity demonstrated herein exemplifies how the reaction pathway changes according to the interaction between the molecules and specific facets of the catalyst. Alternative forms of poisoning may produce varying outcomes.
| Treatment | MI (%) | ADR (%) | ||
|---|---|---|---|---|
| On ZnO powder | On ZnO nanorods | On ZnO powder | On ZnO nanorods | |
| At pH 4 | ||||
| Deionized water | 14.45 ± 0.92 | 14.19 ± 2.38 | ||
| 10 ppm diuron solution | 7.45 ± 1.63 | 29.53 ± 0.77 | ||
| Diuron solution diluted to the concentration corresponding to 1 min degradation | 8.95 ± 2.62 | 9.00 ± 1.84 | 25.14 ± 5.20 | 22.22 ± 1.43 |
| 1 min degradation | 6.55 ± 0.78 | 7.60 ± 0.28 | 38.17 ± 6.74 | 28.95 ± 2.94 |
| 15 min degradation | 10.40 ± 0.28 | 11.05 ± 0.49 | 20.67 ± 1.48 | 16.74 ± 1.17 |
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| At pH 7 | ||||
| Deionized water | 19.70 ± 0.85 | 7.87 ± 0.74 | ||
| 10 ppm diuron solution | 9.45 ± 1.77 | 21.69 ± 1.85 | ||
| Diuron solution diluted to the concentration corresponding to 1 min degradation | 13.50 ± 1.70 | 13.10 ± 0.99 | 12.22 ± 1.48 | 16.79 ± 1.27 |
| 1 min degradation | 10.30 ± 0.14 | 11.45 ± 1.91 | 21.84 ± 1.76 | 20.09 ± 5.25 |
| 15 min degradation | 15.15 ± 0.92 | 18.90 ± 1.84 | 12.54 ± 0.18 | 8.99 ± 2.38 |
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| At pH 10 | ||||
| Deionized water | 12.55 ± 3.04 | 16.33 ± 2.31 | ||
| 10 ppm diuron solution | 6.15 ± 0.92 | 41.46 ± 7.43 | ||
| Diuron solution diluted to the concentration corresponding to 1 min degradation | 8.80 ± 0.85 | 9.00 ± 0.78 | 26.70 ± 9.74 | 20.00 ± 9.69 |
| 1 min degradation | 6.95 ± 0.49 | 8.10 ± 0.85 | 38.13 ± 3.74 | 24.07 ± 3.42 |
| 15 min degradation | 11.30 ± 0.64 | 6.85 ± 0.64 | 19.03 ± 0.81 | 25.55 ± 7.57 |
In general terms, the degradation products using a 1-minute residence time exhibited increased toxicity compared with the reference solution with the same concentration of diuron. This indicated that certain intermediates from direct diuron degradation become more toxic than diuron itself, especially those formed on ZnO powder. Therefore, considering the disappearance of diuron alone is insufficient for the remediation. Extending the degradation time to 15 minutes revealed a substantial reduction in toxicity because of the continuous degradation of both diuron and its degradation intermediates toward more benign compounds. Nevertheless, the crucial impact of the facet-dependent pathway can be clearly observed herein. Although the photocatalytic degradation of diuron on ZnO nanorods generally yields lower toxicity than that on ZnO powder, the product from 15-minute degradation on ZnO nanorods at pH 10 retained toxicity equivalent to the initial diuron solution, even after roughly 75% of diuron had already been degraded. The results not only emphasize the importance of facet-dependent adsorption and its consequence on reaction pathways but also the effect of pH, which could completely alter the adsorption. The design of the effective photocatalyst for proper remediation must incorporate all aspects affecting interactions between the molecules being degraded and the surface of the catalyst.
Overall, the degradation efficiency increased as the pH decreased, with pH 4 yielding the highest photocatalytic degradation efficiency. The fact that pH 10 offered the lowest degradation efficiency despite the enhanced formation of hydroxyl radicals under alkaline conditions and the larger surface area nanorods exhibited comparable degradation efficiency to ZnO powder emphasize the dominant role of adsorption characteristics and surface interactions in degradation kinetics. Toxicity assessment revealed that ZnO nanorods generally yielded lower toxicity in degradation products, except at pH 10, where cytogenotoxicity persisted despite the high degradation efficiency. These findings highlight the importance of surface interactions, which vary according to pH, in designing ZnO-based photocatalysts for effective remediation. Both the degradation efficiency and potential toxicity of the reaction intermediates must be considered in the design process.
For the photocatalytic degradation of diuron, its degradation intermediates and associated toxicity vary significantly across different facets of ZnO and under different pH conditions. ZnO powder exhibited superior degradation performance despite its smaller surface area. The degradation of diuron followed pseudo-first-order kinetics, and the presence of hydroxyl functional groups in almost all detected intermediates suggests that hydroxyl radicals are the primary reactive species responsible for the degradation. Acidic conditions facilitated stronger polar interactions and higher degradation efficiency, while alkaline conditions altered adsorption orientations and reduced the efficiency regardless of the fact that the generation of hydroxyl radicals was enhanced under alkaline conditions. Cytogenotoxicity testing also revealed that certain degradation products formed under alkaline conditions were more harmful than diuron itself.
These findings emphasize that designing an effective photocatalyst for optimal remediation requires considering all factors influencing the interactions between the degrading molecules and the catalyst surface. Furthermore, achieving complete degradation of both the target molecules and their intermediates is essential to mitigating environmental risks. This study underscores the importance of facet-specific considerations and pH effects in catalyst design, providing valuable insights for the development of tailored photocatalytic systems for environmental remediation.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ta00833f |
| This journal is © The Royal Society of Chemistry 2025 |