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B. Di Credico 1 and I. R. Bellobono 2 and M. D'Arienzo 1 and D. Fumagalli 1 and M. Redaelli 1 and R. Scotti 1 and F. Morazzoni 1
Academic Editor:Dionissios Mantzavinos
1, Department of Material Science, INSTM, HINT-COST Project, University of Milano-Bicocca, Via R. Cozzi 55, 20125 Milano, Italy
2, LASA, Department of Physics, University of Milan, Via Fratelli Cervi, 20090 Segrate, Italy
Received 14 March 2015; Revised 8 May 2015; Accepted 12 May 2015; 27 May 2015
This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
1. Introduction
The access to safe drinking water is essential for human well-being and sustainable development. In the last decade, the spread of micropollutant contamination in many freshwater reservoirs is becoming a serious threat for the environment and human health [1, 2]. In fact, pharmaceuticals, for example, analgesics, anti-inflammatories, beta-blockers, antidiabetics, and X-ray contrast media, are partially metabolized by the human body and remain in water resources [3]. Diclofenac (DCF), ciprofloxacin, erythromycin, ibuprofen, and naproxen are the most commonly detected drugs, due to their large use and introduction into the aquatic environment through human and animal excretions, but also resulting from the unused medications if improperly disposed [4]. Since these pharmaceuticals have long half-lives in the environment, they frequently accumulate, reaching biologically active levels [5].
DCF (2-[2,6-(dichlorophenyl)amino]phenyl acetic acid), a nonsteroidal anti-inflammatory drug [6], has a global consumption of 940 tons per year in the form of capsules, suppositories, tablets, and intravenous solution [7]. Since this drug is not completely metabolized after consumption and it is only partially degraded in treatment plants exploiting conventional and advanced cleaning technologies [8], high concentrations (up to 21.6 μ g/L) of DCF have been detected in municipal wastewater effluent, surface water, groundwater, and drinking water [7].
Among the advanced cleaning processes [9-11], TiO2 -promoted photocatalysis seems a very promising approach toward the effective degradation of several pharmaceutical micropollutants [11-14]. Recently, the DCF photocatalytic treatment by different TiO2 -based catalysts has been reported [15, 16]. In all the examined cases, only 85% of DCF conversion was attained; in fact, the DCF degradation pathway is very complex and includes the formation of partially oxidized products with higher toxicity than the parent compound [17].
It is well known that the TiO2 photocatalytic mechanism involves the so-called reactive oxygen species (ROS), that is, hydroxyl radicals ( [figure omitted; refer to PDF] ), hydroperoxyl radical ( [figure omitted; refer to PDF] ), hydrogen peroxide (H2 O2 ), singlet oxygen ( [figure omitted; refer to PDF] ), and superoxide ( [figure omitted; refer to PDF] ) [18-24]. Upon UV-Vis irradiation, TiO2 converts the incoming photons into electron/hole pairs, which can either recombine or migrate to the material surface, where they can generate ROS and activate redox reactions. [figure omitted; refer to PDF] radicals are the most powerful oxidizing species, and they are considered the first responsible for the photodegradation processes in aqueous solution. [figure omitted; refer to PDF] has less oxidizing properties but generates [figure omitted; refer to PDF] , which acts as powerful selective oxidant in the photosensitized transformation of organic substances [25-27]. In particular, organic pollutants including polycyclic aromatic hydrocarbons or chlorophenols, such as DCF, are considerably vulnerable to singlet oxygen since the electrophilic [figure omitted; refer to PDF] species easily oxidizes the electron-rich olefins, dienes, neutral nucleophiles such as amines, and aromatic hydrocarbons anions [28-30]. Nowadays, TiO2 -based photocatalytic treatments of DCF are far from being optimized and a better knowledge of type and amount of ROS implied in the degradation mechanism may provide an effective tool to optimize mineralization.
Moreover, the photodegradation reactions are usually performed by using TiO2 nanoparticles in aqueous suspension (slurry), which causes difficult postuse recovery of the catalyst and requires expensive and time-consuming separation/recycling processes [18, 31]. TiO2 nanoparticles when dispersed in the surrounding environment may be also hazardous, due to their potential inflammatory and cytotoxic effects [32].
In view of the above considerations, the present study reports on the DCF photocatalytic abatement in water, by using anatase nanoparticles with highly reactive crystal surfaces [33-35], either free [36] or suitably immobilized in a highly porous silica matrix [37].
Anchoring these nanocrystals onto the highly porous silica channels of the TiO2 -SiO2 composite (TS) provides easy accessibility of surface sites as well as easy adsorption/interaction of the drug. Minimum deactivation, thermal stability, no TiO2 leaching, and an easy scale-up of the process for domestic/civil water treatments are also important advantages associated with the employment of this immobilized catalyst.
The degradation of DCF and its transformation products was followed by UV-Vis spectroscopy, being able to identify the most persistent transformation products. The complete photomineralization was assessed by measuring the total organic carbon (TOC) at different reaction times. The ROS species, [figure omitted; refer to PDF] and [figure omitted; refer to PDF] , formed by UV irradiation of the catalysts, were detected by Electron Paramagnetic Resonance (EPR) spin-trap technique. The ROS formation rate and their amount were related to the photoefficiency of both catalysts. Singular and unexpected stability properties have been found for the oxygenated radicals in TS, elucidating a role of the immobilization procedure in preserving the functional properties of the photoactive oxide.
2. Materials and Methods
2.1. Chemicals
DCF sodium salt and all chemicals were purchased from Sigma-Aldrich and used as received without further purification. Milli-Q water (MQ, resistivity 18.2 MΩ·cm at 25°C and TOC <= 5 μ g/L) was used for the procedures that require water.
2.2. Synthesis and Functionalization of TiO2 Nanoparticles
Anatase nanocrystals were obtained according to a previously reported procedure [36]. The TiO2 surface was then functionalized with 2-methoxyethylamine by refluxing the suspension of the oxide with the organic reagent [37].
2.3. Preparation of TiO2 -SiO2 Composite
As reported in our previous study [37], TS was prepared by inducing the sol-gel transition of the SiO2 precursor, tetramethylortosylicate (TMOS), in the presence of the functionalized TiO2 nanoparticles and polyethylene glycol, PEG (see Figure S1 in Supplementary Material available online at http://dx.doi.org/10.1155/2015/919217).
In the present study, TS composite was produced with a pellet shape, in order to be handily used in reactor and plants. Pellets were obtained by casting the precursor sol-phase in a suitable Teflon mold, constituted by several separated cylindrical holes (average diameter and average depth 0.5 cm). After ageing, the gel phase filling the holes was dried at 150°C for 1 h and finally calcined in air at 500°C for 5 h. This allows us to obtain TS pellets where TiO2 nanocrystals lie at the surface of macroporous cavities inside the SiO2 matrix.
2.4. Morphological and Chemical Characterization of TiO2 Nanoparticles and TS Composite
The structure and the morphological features of both TiO2 nanoparticles and TS composite were checked by using X-Ray Diffraction (XRD), Scanning Electron Microscopy (SEM), and Transmission and High-Resolution Transmission Electron Microscopy (TEM/HRTEM). The experimental conditions and the analytical details are previously reported [36, 37]. Specific surface area (SSA) and pore size distribution of micro- and mesopores were also checked in both TiO2 and TS samples and compared to the previously reported results [36, 37].
2.5. Photoinduced Degradation of DCF
Photodegradation experiments employing TiO2 nanoparticle slurry as catalyst were carried out in a 600 mL Pyrex discontinuous batch reactor with an external cooling jacket enveloped by an aluminum foil, equipped with a UV-Vis lamp placed in a coaxial quartz cylinder. The 125 W Hg high pressure lamp was used for UV-visible excitation (emission lines at [figure omitted; refer to PDF] , 313, 366 (main), 405, and 436 nm). No optical filter was adopted. The photocatalytic experiments were carried out by using the DCF concentrations 2.0, 20.0, and 50 mg/L to confirm the reaction mechanism, the kinetics of the process, and the reaction products. Titania nanocrystals ( [figure omitted; refer to PDF] mg, 0.25 g L-1 ) were suspended by ultrasound in 600 mL of water containing DCF at the concentrations reported above and recirculated by a peristaltic pump (14 mL s-1 ). The temperature was kept at [figure omitted; refer to PDF] °C.
When employing TS, the pellets were arranged inside the cylindrical photoreactor, shown in Figure 1, to facilitate both direct and diffuse light irradiation. For the photocatalytic experiments, 600 mL of water containing DCF at the concentrations reported above was recirculated in the presence of approximately [figure omitted; refer to PDF] g of TS (TiO2 loading 0.128 g, corresponding to 0.21 g L-1 ) as described in Figure 1(b) [38].
Figure 1: (a) Scheme of the photoreactor and the arrangement of the porous TS pellets (lateral and vertical cross-section views). (b) Schematic view of the photocatalytic plant.
(a) [figure omitted; refer to PDF]
(b) [figure omitted; refer to PDF]
The photocatalytic experiments were carried out also employing TS powder in slurry. In all cases, the aqueous phase was saturated by continuously bubbling oxygen (constant feed = 100 mL min-1 ) in an online chamber and circulated in the dark for 30 min before turning on the UV-Vis source. The excess of gas was eliminated through nonreturn check valve. Control experiments were carried out in the absence of TiO2 (Blank). The photocatalytic degradation was followed firstly by UV-Vis spectroscopy. Aliquots (6 mL) of the reaction solution were drawn out at regular intervals, and the centrifuged clear solutions were utilized to record the spectra under the following conditions: wavelength range: 190-400 nm, scan rate: 600 nm min-1 , time response: 0.1 s, and spectral band: 2 nm (Varian Cary 4000 Spectrophotometer). The DCF complete mineralization was analyzed by measuring TOC with a Shimadzu TOC-V CSH analyzer.
2.6. Spin-Trap EPR Experiments
Spin-trap experiments were performed to detect the short-living ROS, namely, [figure omitted; refer to PDF] , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] , in the reaction aqueous medium. The reagent to reveal the [figure omitted; refer to PDF] species was 2,2,6,6-tetramethyl-4-piperidine (TEMP), whereas 5,5-dimethyl-1-pyrroline-N-oxide (DMPO) simultaneously detects [figure omitted; refer to PDF] , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] . In order to distinguish the contribution of [figure omitted; refer to PDF] and [figure omitted; refer to PDF] , from that of [figure omitted; refer to PDF] , a typical [figure omitted; refer to PDF] radical scavenger, DMSO (50 mM), was employed. Spectra were acquired before and during the UV-Vis irradiation in the EPR cell.
The stock suspensions were prepared by dispersing TiO2 and TS in powder form in MQ water (20 mM in TiO2 ) and carefully homogenizing them in ultrasound bath (1 h). Then, the appropriate spin-trap agent (concentration: 20 mM) was added.
The stock solution in a reservoir was purged for 30 min with pure O2 before the experiment and then, just a few minutes before irradiation, was pumped into the EPR cell (6 cm window length, 0.5 mm optical path) through a Teflon tube directly connected to the reservoir. EPR investigation was performed at 293 K by a Bruker EMX spectrometer working at the X-band frequency. The irradiation source was a UV-Vis 150 W Xe lamp with the output radiation focused on the samples in the cavity by an optical fiber (50 cm length, 0.3 cm diameter). The [figure omitted; refer to PDF] values were calculated by standardization with α ,α [variant prime]-diphenyl-β -picrylhydrazyl (DPPH).
Typical EPR spectrometer settings were microwave frequency 9.8 GHz; microwave power 10 mW; sweep width 6-10 mT; modulation amplitude 0.05-0.2 mT; scan time 20.97 or 41.94 s; time constant 40.96 or 81.92 ms.
The maximum intensity of the first derivative peak of the spin-trapped signal was plotted against the reaction time in order to follow the ROS production in the irradiated suspensions. The initial slope ( [figure omitted; refer to PDF] ), calculated as tangent of the curve at the beginning of the adduct formation, was taken as representative parameter [26] of the ROS formation rate.
3. Results and Discussion
3.1. Structural and Morphological Characterization of TiO2 and TS Catalysts
XRD patterns of both TiO2 and TS catalysts indicate the exclusive presence of the anatase phase (Figure S2).
In order to check the correspondence with the solids reported in our previous paper [36], TEM and HRTEM images of TiO2 nanocrystals were collected (Figure 2(a)). No internal pores or amorphous surface layers were detectable. Particles show almost square or rectangular shapes with aspect ratio [figure omitted; refer to PDF] ( [figure omitted; refer to PDF] = length/width) of about 1-3.
Figure 2: TEM and HRTEM images of TiO2 (a) and TS composite (b, c). Details on crystallographic planes detected are shown in the inset of (a) and (c).
(a) [figure omitted; refer to PDF]
(b) [figure omitted; refer to PDF]
(c) [figure omitted; refer to PDF]
Higher magnification (inset in Figure 2(a)) of the lattice fringes along the [figure omitted; refer to PDF] direction clearly reveals the presence of (002) crystallographic planes with lattice space of 0.48 nm. This indicates that TiO2 nanocrystals mainly expose the high-energy [figure omitted; refer to PDF] and [figure omitted; refer to PDF] facets, even if smaller amounts of thermodynamically stable and lower energy [figure omitted; refer to PDF] surfaces are detectable (see further TEM and HRTEM images in Figure S3). According to the literature [39-42], anatase [figure omitted; refer to PDF] , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] faces are thought to be differently involved in the photooxidation, due to their different surface energy, and are responsible for the high reactivity of hydrothermal TiO2 [18, 34, 41]. In particular, the [figure omitted; refer to PDF] surfaces display the highest density of undercoordinated Ti centers and enlarged O-Ti-O bond angles, which increases the surface energy and makes titanium and oxygen centers very reactive in photooxidation reactions [39, 41]. In addition, we have recently proved that also the [figure omitted; refer to PDF] surfaces contribute to the oxidation processes via the formation of the superoxide species [41]. Besides, Pan et al. [34] reported that particles, where the [figure omitted; refer to PDF] surfaces are copresent with a high percentage of [figure omitted; refer to PDF] facets, promote the generation of OH radicals.
The morphology of TS was also investigated and compared with the results of our previous study. SEM micrographs (Figure S4) show that the average diameter of silica particles in the matrix is about 2.5 μ m and confirm the presence of an interconnected macroporous structure. TEM and HRTEM images of TS (Figures 2(b) and 2(c)) show that TiO2 nanocrystals are anchored to the surface of silica channels without forming large aggregates and maintain their pristine size, shape, and exposed [figure omitted; refer to PDF] , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] crystals facets (inset in Figure 2(c)).
Nitrogen physisorption experiments performed on TS samples revealed the occurrence of a type IV isotherm with a wide hysteresis loop, suggesting a remarkable mesopores contribution (Figure S5) to the total surface area. The pore size distribution (inset in Figure S5) supports the existence of mesopores, due to the TiO2 nanocrystals [37], with an average pore diameter centred at 3.6 nm.
3.2. Photodegradation of DCF: UV-Vis Spectroscopy Investigation
The photodegradation of DCF in the presence of TiO2 or TS was firstly followed by UV-Vis absorption spectroscopy (Figures 3(a) and 3(b)), compared to that in the absence of catalyst (see Figure S6). Several DCF transformation products were identified.
Figure 3: Selected absorption spectra of DCF recorded at different reaction times in the presence of (a) TiO2 and (b) TS. (DCF (solid line), with photoreaction spectra after 2 min (dashed line), 10 min (dotted line), and 120 min (dotted-dashed line)). (c) Photodegradation pathway proposed for DCF in the presence of TiO2 and TS catalysts with hypothesized carbazole intermediates , shown in square brackets .
(a) [figure omitted; refer to PDF]
(b) [figure omitted; refer to PDF]
(c) [figure omitted; refer to PDF]
In the case of pure TiO2 , the absorption spectrum of DCF initially (time = 0 min) shows a single band centred at 279 nm (solid line in Figure 3(a)). This feature disappears after 2 min of UV-Vis irradiation (dashed lines in Figure 3(a)) and simultaneously four new bands at 210, 240, 289, and 324 nm become detectable (dashed lines in Figure 3(a)). According to the literature [43], these features can be unambiguously assigned to the monohalogenated carbazole (DCF-DP1, Figure 3(c)), resulting from the loss of one chlorine atom followed by intramolecular cyclization of DCF.
After 10 min of irradiation, the DCF-DP1 absorption peaks gradually decrease in intensity (dotted lines in Figure 3(a)) and slightly shift toward higher wavelengths. This may suggest that the chromophoric carbazole structure remains basically unaffected along the reaction time, and the photodegradation probably progresses through the formation of the DCF-DP2 and DCF-DP3 intermediates (Figure 3(c)), as already observed in the literature under similar reaction conditions [3, 43]. DCF-DP2 and DCF-DP3 products have in fact a carbazole-based structure whose [figure omitted; refer to PDF] -conjugated condensed rings possess high stability and therefore are recalcitrant to further degradation. The formation of carbazoles, recently assessed for DCF photobiodegradation in an aquatic environment under solar light irradiation, is particularly undesired due to their remarkable phytotoxicity [44]. After 120 min reaction time, the spectral features attributed to carbazole species became very weak and poorly resolved (dotted-dashed line in Figure 3(a)).
In the presence of TS catalyst, a similar spectral behavior has been observed (Figure 3(b)). In this case, the starting drug was transformed in DCF-DP1 after a higher irradiation time (10 min) than that for pure anatase (dotted lines in Figure 3(b)). However, the spectrum shows that the immobilized system was able to remove DCF and its recalcitrant photoproducts after 120 min (dotted-dashed line in Figure 3(b)), as well as the pure TiO2 in slurry.
On the contrary, in the Blank experiment (Figure S6), the UV-Vis spectra show intense and very stable peaks relatable to DCF-DP1 and DCF-DP2 till the end of the reaction time.
This suggests that the utilized catalysts favour the breakdown of the carbazole structures and the complete drug degradation.
3.3. Photomineralization of DCF: TOC Analysis
In order to assess the complete mineralization of DCF, a TOC analysis was performed. During the initial stage of recirculation in the dark (30 min), the chemisorption of the drug on the catalyst surface caused a TOC depletion of about [figure omitted; refer to PDF] %. The experimental data obtained by using either TiO2 or TS are shown in Figure 4. The Blank test is also reported for comparison.
Figure 4: Mineralization curves (given as TOC%) of DCF (50 mg/mL) under UV-Vis irradiation in the presence of O2 for ([...]) Blank, ([white circle]) TiO2 , and ([...]) TS in slurry.
[figure omitted; refer to PDF]
For TiO2 nanocrystals, a sharp decrease of the TOC percentage is observed in the first 10 min of the reaction. After 30 min, the degradation apparently brakes and then, only at higher reaction times ( [figure omitted; refer to PDF] min), a sharp TOC decay again occurs. In the case of TS composite, the DCF photodegradation is initially slow, while after a reaction time of 50 min a significant decay of the TOC amount is noticeable (Figure 4).
These results are consistent with the degradation mechanism proposed for DCF on the basis of UV-Vis analysis. In the presence of TiO2 nanocrystals, the sharp decrease of the TOC percentage in the first minutes of the process corresponds to the formation of subproducts, probably deriving from DCF decarboxylation and/or dealkylation reactions. Afterwards, the decrease of the degradation rate, observed at different reaction times for TiO2 and TS samples, may be attributed to the persistent presence of hypothesized halogenated carbazole (DCF-DP1) and of DCF-DP2 and DCF-DP3 carbazole molecules and to their recalcitrant phototransformation products, which presumably originate from the loss of the carboxylic group and the alkyl chain, followed by the breaking of aromatic rings and formation of alkane derivatives. This behavior is more remarkable and evident for TS, rather than TiO2 alone. However, at the end of the process, DCF is completely mineralized by both employing TS and TiO2 catalysts, whereas the degradation is negligible under simple photolytic condition (Figure 4).
It is interesting to note that the complete mineralization of the drug occurs in very similar times for both TiO2 and TS catalysts. This is again in agreement with the UV-Vis results and demonstrates the efficacy of the immobilization procedure in preserving the peculiar photoactivity of TiO2 . The same behavior has already been observed in the photomineralization of the phenol [18, 37] and was ascribed to the high dispersion of catalyst nanocrystals at the surface of silica macropores, which guarantees high accessibility of the catalyst at the solid-liquid interface and intimate contact between the substrate molecules and the nanoparticles.
In order to compare the mineralization kinetics of DCF using TiO2 or TS catalysts, the half degradation time ( [figure omitted; refer to PDF] ), that is, the reaction time at which the TOC reaches 50%, was used as the representative parameter. Even if the best catalytic performance occurs for pure TiO2 ( [figure omitted; refer to PDF] min), the TS composite displays an efficiency ( [figure omitted; refer to PDF] min) much higher than the Blank (estimated [figure omitted; refer to PDF] min). These results suggest that the utilization of anatase nanocrystals with [figure omitted; refer to PDF] , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] exposed surfaces, either free or immobilized in silica matrix, can enhance the photooxidation reactions, even for those of the very stable substrates like DCF or carbazoles. The negligible DCF degradation is in the absence of catalyst and is in agreement with the reported high stability of DCF, for which complete photomineralization is difficult to achieve by conventional water treatments [15-17].
The satisfactory performances of immobilized catalyst confirm that the immobilization procedure preserves the catalytic properties of TiO2 even for the abatement of the highly stable pharmaceuticals and simultaneously guarantees the benefits related to the use of a supported catalyst.
3.4. Kinetics of DCF Photodegradation for TS Composite and TiO2 Nanocrystals
In order to obtain deeper insight into the photodegradation mechanism, the four-parameter kinetic model, proposed by Rota et al. for the partly heterogeneous oxidation of different complex organic substrates [45], was here applied to the DCF photomineralization (50 mg/L) catalyzed by either TiO2 nanocrystals or TS composite.
According to this model, the DCF mineralization to CO2 was assumed to occur through a single intermediate I, which contains the contribution of all intermediates: [figure omitted; refer to PDF] A system of first-order differential equations describes the variation of DCF, I, and CO2 concentrations [46, 47]: [figure omitted; refer to PDF] where [figure omitted; refer to PDF] , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] are the concentrations of DCF, I, and CO2 ; [figure omitted; refer to PDF] and [figure omitted; refer to PDF] are the apparent chemisorption constants related to the competitive absorption of DCF and I, respectively, onto TiO2 surface, and [figure omitted; refer to PDF] and [figure omitted; refer to PDF] represent the kinetic constants of the DCF and I degradation.
According to Figure 4, when the photodegradation in the presence of TS composite starts, [figure omitted; refer to PDF] is negligible with respect to [figure omitted; refer to PDF] , and the kinetic equations can be approximated to [figure omitted; refer to PDF] At the beginning of the process, the term [figure omitted; refer to PDF] ( [figure omitted; refer to PDF] M and the order of magnitude of [figure omitted; refer to PDF] for DCF may be assumed very high) and (4) can be further simplified to a pseudo zero-order kinetic equation: [figure omitted; refer to PDF] where [figure omitted; refer to PDF] is the pseudo zero-order kinetic constant.
Integrating between reaction times [figure omitted; refer to PDF] and [figure omitted; refer to PDF] results in [figure omitted; refer to PDF] Considering that at the very early stages of reaction the total organic carbon concentration may be assumed [figure omitted; refer to PDF] C, as DCF contains 14 carbon atoms, and that the very small concentrations of intermediates have structures very similar to the parental drug, (5) can be written as follows: [figure omitted; refer to PDF] by expressing the DCF concentration in terms of carbon concentration.
Coherently, the plot of ( [figure omitted; refer to PDF] ) versus reaction time ( [figure omitted; refer to PDF] ) for the photodegradation of DCF in the presence of TS composite proves that, for reaction times below 50 min, the reaction follows an apparent zero-order (Figure 5(a)).
Figure 5: Plots of (a) ( [figure omitted; refer to PDF] ) and (b) [figure omitted; refer to PDF] versus reaction time calculated from the experimental TOC versus time curves of DCF photomineralization in the presence of TS composite, according to (6) and (10).
(a) [figure omitted; refer to PDF]
(b) [figure omitted; refer to PDF]
On the other hand, at a time [figure omitted; refer to PDF] min, when [figure omitted; refer to PDF] , the kinetic equation (6) can be simplified to the following: [figure omitted; refer to PDF] When [figure omitted; refer to PDF] is very small, (7) becomes a pseudo first-order kinetic equation, where [figure omitted; refer to PDF] is the pseudo first-order kinetic constant: [figure omitted; refer to PDF] By integrating between [figure omitted; refer to PDF] and [figure omitted; refer to PDF] we obtain [figure omitted; refer to PDF] By considering that when [figure omitted; refer to PDF] , [figure omitted; refer to PDF] and that [figure omitted; refer to PDF] , (9) can be rewritten as [figure omitted; refer to PDF] Reporting the [figure omitted; refer to PDF] versus reaction time ( [figure omitted; refer to PDF] ), the first-order kinetics can be easily observed (Figure 5(b)). According to (6) and (10), [figure omitted; refer to PDF] and [figure omitted; refer to PDF] have been calculated from the slopes of the straight lines fitting the experimental points and reported in Table 1.
Table 1: Kinetic constants of TiO2 nanocrystals and TS composite for the photomineralization of DCF.
Sample | [figure omitted; refer to PDF] (mol min-1 ) | [figure omitted; refer to PDF] (min-1 ) | [figure omitted; refer to PDF] (min-1 ) | [figure omitted; refer to PDF] (min-1 ) | [figure omitted; refer to PDF] (min-1 ) |
TiO2 | n.o. [figure omitted; refer to PDF] | n.o. | 1.3 × 10-2 | 3.5 × 10-3 | 1.4 × 10-2 |
TS | 5.0 × 10-6 | 1.2 × 10-2 | n.o. | n.o. | n.o. |
[figure omitted; refer to PDF] Not observed.
When the reaction is catalyzed by TiO2 nanocrystals, the DCF degradation trend is different from that of TS (see Figure 4) and essentially follows an apparent first-order kinetics law. In fact, at the beginning of the process ( [figure omitted; refer to PDF] min), [figure omitted; refer to PDF] rapidly increases and therefore [figure omitted; refer to PDF] . Consequently, a pseudo first-order kinetic law with a [figure omitted; refer to PDF] ((8)-(9)) effectively describes the initial steps of the reaction. For [figure omitted; refer to PDF] min, the degradation slows down, but again an apparent first-order kinetics with a constant [figure omitted; refer to PDF] , lower than [figure omitted; refer to PDF] , is the representative of the process. Finally, for a reaction time [figure omitted; refer to PDF] min, the kinetic behavior for TiO2 sample becomes very similar to that of TS; [figure omitted; refer to PDF] can be defined. Figure 6 shows the plot of the [figure omitted; refer to PDF] versus reaction time ( [figure omitted; refer to PDF] ) for the DCF degradation in the presence of TiO2 nanocrystals. The values of the three different pseudo first-order kinetic constants have been calculated from the slopes of the straight lines fitting the experimental points and reported in Table 1.
Figure 6: Plots of [figure omitted; refer to PDF] versus reaction time calculated from the experimental TOC versus time curves of DCF photomineralization in the presence of TiO2 nanocrystals, according to (6) and (10).
[figure omitted; refer to PDF]
Since the kinetic behaviors of the samples are very different for reaction times lower than 120 min, a fair comparison cannot be made by considering only the rate constants values, owing also to the above observations concerning the greater efficiency of TiO2 with respect to TS and to the concentration effects, which may be different for intermediates of photodegradation in the different stages of the overall photocatalytic degradation process. However, it can be observed that the presence of first-order kinetics for TiO2 nanocrystals is in agreement with its higher [figure omitted; refer to PDF] time in the DCF photomineralization.
3.5. Study of ROS Species in the Presence of TiO2 and TS Catalysts
The UV irradiation of TiO2 in oxygenated aqueous media results in the generation of ROS ( [figure omitted; refer to PDF] , H2 O2 , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] ), which are thought, at the molecular level, to be the active intermediates of the photooxidation processes [20-24]. Among them, [figure omitted; refer to PDF] has the highest oxidation potential (E°( [figure omitted; refer to PDF] /H2 O) = +2.27 V versus NHE at pH 7) [48], and it is believed to be the main responsible species for the photooxidation processes in aqueous solution. The photoproduced H2 O2 also contributes to the formation of [figure omitted; refer to PDF] species, since it is rapidly photolyzed by UV irradiation. [figure omitted; refer to PDF] is instead a lower oxidant (E°( [figure omitted; refer to PDF] / [figure omitted; refer to PDF] ) = +0.34 V [49], while superoxide is essentially a poor oxidant E°(O2 / [figure omitted; refer to PDF] ) = -0.28 V) [48]. Since both [figure omitted; refer to PDF] and [figure omitted; refer to PDF] demonstrate important selectivity in several reported photooxidative processes [26-30], it appears mandatory to investigate the nature and the amount of these species in our process.
A very suitable in situ method to determine these species exploits the spin-trapping agents, by using EPR for detection, due to the short ROS life times. The identification of hydroxyl radicals is usually performed by using DMPO as reactive probe [50-52]. The interaction of [figure omitted; refer to PDF] species with DMPO yields the [figure omitted; refer to PDF] adduct (inset in Figure 7(a)). [figure omitted; refer to PDF] displays a four-line EPR signal with Hamiltonian parameter [figure omitted; refer to PDF] and hyperfine splitting, [figure omitted; refer to PDF] mT, [figure omitted; refer to PDF] mT (Figure 7(a)), in agreement with a very large number of references [50, 51].
Figure 7: (a) EPR spectrum of the DMPO-OH adduct (structure shown in the inset). (b) Variation of the DMPO-OH resonance lines with the UV-Vis irradiation time for the TS aqueous suspension.
(a) [figure omitted; refer to PDF]
(b) [figure omitted; refer to PDF]
Recent studies [52, 53] have suggested that DMPO, in addition to reacting with [figure omitted; refer to PDF] , can be oxidized by [figure omitted; refer to PDF] and [figure omitted; refer to PDF] to yield [figure omitted; refer to PDF] . Therefore, DMPO cannot selectively trap [figure omitted; refer to PDF] , while it simultaneously reveals hydroxyl, superoxide, and singlet oxygen.
Aiming to find significant relationships between the presence of different ROS and the photoactivity of TiO2 -based catalysts in DCF photodegradation, the following experiments were performed.
Firstly, EPR spectra were recorded under UV-Vis irradiation in the presence of DMPO. In order to evaluate the contribution of superoxide and singlet oxygen to the [figure omitted; refer to PDF] signal, experiments were also performed in the presence of DMSO, a typical [figure omitted; refer to PDF] quencher [54].
At the beginning of irradiation, the [figure omitted; refer to PDF] adduct rapidly forms for both TiO2 and TS catalysts, and the signal intensity increases over time (Figures 7(b) and 8(a)).
Figure 8: (a) Time course of the [figure omitted; refer to PDF] signal maximum before and during UV-Vis irradiation for TiO2 (black line) and TS (red line) samples; (b) magnification of the initial portion of the curve for which the initial slope ( [figure omitted; refer to PDF] ) was taken as representative parameter to evaluate the initial rate of [figure omitted; refer to PDF] , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] generation.
(a) [figure omitted; refer to PDF]
(b) [figure omitted; refer to PDF]
However, prolonged irradiation results in a decrease of the [figure omitted; refer to PDF] amount, probably due to the coupling of the radicals and/or to progressive oxidation of DMPO, as a result of the multiple addition of OH radicals producing EPR-silent products (Figure 8(a)) [51, 55, 56].
Thus, the maximum intensity of the EPR signal cannot be univocally associated with the amount of the ROS species and the initial slope [figure omitted; refer to PDF] of the [figure omitted; refer to PDF] curve intensity versus time, corresponding to the initial rate of [figure omitted; refer to PDF] , [figure omitted; refer to PDF] , and [figure omitted; refer to PDF] formation (Figure 8(b)), was assumed as representative parameter.
Figure 8(b) shows that the TiO2 has a higher [figure omitted; refer to PDF] value than the TS sample, in agreement with the better performance observed for the titania nanocrystals in DCF photodegradation. However, comparing the curves in Figure 8(a), it must be highlighted that after 240 seconds the generation of [figure omitted; refer to PDF] species undergoes a fast decay in the presence of TiO2 catalyst (black line), whereas for the TS catalyst it remains constant for at least 600 seconds since the beginning of the UV-Vis irradiation (red line).
This suggests that the quenching of [figure omitted; refer to PDF] radicals is inhibited in the titania-silica composite. We may attribute such effect to the high macro-/mesoporosity of the silica channels which tune the DMPO/ [figure omitted; refer to PDF] diffusion toward/from the catalytic active sites, thus making gradual their interaction with the highly dispersed TiO2 nanocrystals. This may prevent either the coupling or the fast photooxidation of [figure omitted; refer to PDF] radicals. On the basis of the previous observations, we suggest that the anatase nanoparticles act as confined "nanoreactors," where the ROS species are formed and may easily interact with the DCF molecules before their annihilation.
After the addition of DMSO, a typical [figure omitted; refer to PDF] radical quencher, to the aqueous suspensions of TiO2 and TS, only a partial decrease of the [figure omitted; refer to PDF] signal was observed, while additional features attributable to DMPO-CH3 (with hyperfine constant [figure omitted; refer to PDF] mT, [figure omitted; refer to PDF] mT, Figure 9) appear. This suggests that the generation of [figure omitted; refer to PDF] adduct upon UV-Vis irradiation of TiO2 and TS derives from the trapping of ROS other than [figure omitted; refer to PDF] . These radicals being stable in the presence of DMSO may be attributed mainly to the oxidation of DMPO operated by singlet oxygen (deriving from [figure omitted; refer to PDF] ), indicating a possible contribution of this species to the photodegradation mechanism.
Figure 9: Effect of DMSO on the [figure omitted; refer to PDF] signal during UV-Vis irradiation of aqueous suspensions of TiO2 and TS.
[figure omitted; refer to PDF]
While many papers support the relevance of [figure omitted; refer to PDF] in TiO2 -assisted photocatalytic processes [54-57], only few of them comprehensively describe the role of singlet oxygen species when the catalyst is immobilized [58].
Aiming to confirm the presence of this highly oxidant species in TiO2 and TS suspensions, a second set of EPR experiments was carried out by using the TEMP spin trap, being able to evidence the [figure omitted; refer to PDF] species, giving the TEMPO radical (inset in Figure 10(a)) [59].
Figure 10: (a) Variation of resonance lines of the TEMPO radical (structure shown in the inset), with the UV-Vis irradiation time for the TS aqueous suspension; (b) time course of the TEMPO signal maximum before and during UV-Vis irradiation for TiO2 (black line) and TS (red line) samples. The initial slope ( [figure omitted; refer to PDF] ) of the curve was taken as representative parameter to evaluate the initial rate of [figure omitted; refer to PDF] formation.
(a) [figure omitted; refer to PDF]
(b) [figure omitted; refer to PDF]
The obtained 2,2,6,6-tetramethyl-4-piperidone-N-oxyl (TEMPO) species is characterized by a typical three-line EPR signal with hyperfine constant [figure omitted; refer to PDF] mT and [figure omitted; refer to PDF] .
Figure 10(a) shows the EPR spectra in the presence of TEMPO during the first 180 seconds of UV-Vis irradiation of TS suspensions. Similar results are obtained for TiO2 (not shown). As already observed for the [figure omitted; refer to PDF] , the TEMPO signal decreases in intensity along the irradiation time (Figure 10(b)); as a consequence, the initial slope [figure omitted; refer to PDF] of the TEMPO signal versus time was used as the representative parameter to evaluate the initial rate of [figure omitted; refer to PDF] formation.
Also in this case, the [figure omitted; refer to PDF] value for pure TiO2 is higher than the value for TS (Figure 8(b)), in accordance with the photocatalytic performances of the samples. The generation of TEMPO radicals in TiO2 suspension increases up to ~500 sec. and then rapidly decreases. Instead, in the presence of TS, the formation of radicals increases up to 700 sec. and then remains constant till the end of the irradiation time. This indicates, in analogy to the behavior of [figure omitted; refer to PDF] radicals, a higher stability of TEMPO radicals in TS composite than in TiO2 and suggests that the coupling of TEMPO radicals is inhibited in TS due to the TiO2 dispersion.
These results confirm a significant involvement of singlet oxygen in the photodegradation mechanism. In particular, the presence of [figure omitted; refer to PDF] species may be associated with the enhanced degradation of DCF and with the decomposition of its carbazole oxidation products. In fact, [figure omitted; refer to PDF] acts as an elective oxidant of electron-rich aromatic intermediate [43, 44], favoring their complete degradation.
In the present study, the formation rate and the concentration of different spin-trapped species have been used to measure the ROS yield and are connected to the catalytic behavior of the TiO2 and TS samples. However, these data cannot be directly related to the degradation pathway of DCF because the spectra were acquired in the absence of the drug. Nevertheless, our investigation clearly demonstrates that a fair study of the titania-assisted photodegradation of pharmaceuticals must take into account the type, amount, and life time of different ROS species in order to understand the occurrence of specific catalytic performance.
4. Conclusions
The present study reports the oxidative photocatalytic degradation of 2-[2,6-(dichlorophenyl)amino]phenylacetic acid, DCF, in the presence of hydrothermal TiO2 and TS materials as catalysts. The reaction was studied by UV-Vis absorption spectroscopy and by TOC determination.
It turned out that both TiO2 and the TS composite display a remarkable efficiency in the degradation of the drug. Indeed DCF and its intermediate products, which resulted in being very stable under conventional and advanced water treatment, have been completely mineralized.
These results support the idea that the utilization of anatase nanocrystals with highly reactive exposed surfaces can be an effective tool for enhancing photooxidation reactions, even those of stable and persistent organic pollutants like DCF. Furthermore, the TiO2 here employed, immobilized in silica matrix, preserves the functional properties of the unsupported active oxide, while allowing an easy technical use and recovery of the catalyst.
The catalysts performances have been related to the presence of three types of reactive oxygen species during the reaction, hydroxyl radicals ( [figure omitted; refer to PDF] ), singlet oxygen ( [figure omitted; refer to PDF] ), and superoxide ( [figure omitted; refer to PDF] ). The formation of these ROS, assessed by EPR spin-trap experiments, indicates the significant involvement of singlet oxygen species in the DCF photodegradation.
It has also been suggested that ROS species do not easily quench in the titania-silica composite, thus increasing their possibility to be effective in the photodegradation process. This behavior may be ascribed to the high macro-/mesoporosity of the silica channels which tune the DMPO/ [figure omitted; refer to PDF] diffusion toward/from the catalytic active sites, thus making gradual their interaction with the highly dispersed TiO2 nanocrystals. This may prevent either the coupling or the fast photooxidation of [figure omitted; refer to PDF] radicals.
The nanocrystals act therefore as confined "nanoreactors," where ROS species form and can readily interact with the pollutants molecules.
To sum up, the substantially equal efficiencies of TiO2 alone and TS, if referred to global mineralization times when mineralization is completed, may be attributed, if not solely at least predominantly, to the stabilization effect of ROS by TS, in agreement with EPR results, which is able to change its kinetics in the early stage of photocatalytic mineralization process.
These innovative and unexpected properties of stabilization of oxygenated radicals exerted by the TS composite highlight the role of the reported immobilization procedure in preserving the functional properties of the photoactive oxide.
Acknowledgments
This work was in the frame of the European COST action MP1202 "Rational Design of Hybrid Organic Inorganic Interfaces: The Next Step towards Advanced Functional Materials." The authors thank Professor Stefano Polizzi of the University of Venezia for TEM analysis. M. Redaelli thanks Corimav for its support within the PCAM European Doctoral Programme.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
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Abstract
We report on the photodegradation of diclofenac (DCF) by hydrothermal anatase nanocrystals either free or immobilized in porous silica matrix (TS) in connection to the type and amount of reactive oxygen species (ROS), in order to have deeper insight into their role in the photocatalysis and to provide an effective tool to implement the DCF mineralization. TiO2 and TS exhibit a remarkable efficiency in the DCF abatement, supporting that the utilization of anatase nanoparticles with the highly reactive {001}, {010}, and {101} exposed surfaces can be an effective way for enhancing the photooxidation even of the persistent pollutants. Furthermore, the hydrothermal TiO2, when immobilized in silica matrix, preserves its functional properties, combining high photoactivity with an easy technical use and recovery of the catalyst. The catalysts performances have been related to the presence of OH*, [subscript]O2[/subscript] 1, and [superscript][subscript]O2[/subscript] -*[/superscript] species by electron paramagnetic resonance spin-trap technique. The results demonstrated that the ROS concentration increases with the increase of photoactivity and indicated a significant involvement of [subscript]O2[/subscript] 1 in the DCF degradation. The efficacy of TiO2 when immobilized on a silica matrix was associated with the high ROS life time and with the presence of singlet oxygen, which contributes to the complete photomineralization of DCF.
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