Immobilized TiO2 on glass spheres applied to heterogeneous photocatalysis: photoactivity, leaching and regeneration process

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Heterogeneous photocatalysis using titanium dioxide (TiO2) has been widely investigated as an attractive advanced oxidation process for the physicochemical treatment of a variety of pollutants in water (Malato et al., 2003; Hashimoto, Irie & Fujishima, 2005; Pelaez et al., 2012; Chen et al., 2015; Han et al., 2017; Manassero, Satuf & Alfano, 2017; Nur et al., 2017; Srikanth et al., 2017). TiO2 is one of the most used catalysts in photocatalytic degradation of organic pollutants due to properties such as absence of toxicity, very low solubility, high chemical and photostability and low cost (Machado et al., 2012; Wang et al., 2012). Moreover, TiO2 absorbs non-negligible portions (3–4%) of available solar energy at the Earth’s surface (Spasiano et al., 2015).

When the absorbed photon energy is equal to or higher than the band gap energy of the semiconductor catalyst, electron–hole pairs are generated. This electron–hole pair has a high and sufficiently positive potential to induce the formation of hydroxyl radicals from water molecules and hydroxyl (OH) ions adsorbed on the semiconductor surface. Hydroxyl radical is the most powerful oxidizing species after fluorine and it can degrade many pollutants due to its low selectivity (Machado et al., 2012; Kim et al., 2016).

The heterogeneous photocatalysis process using TiO2 as catalyst in aqueous matrices can be carried out in a slurry reactor or TiO2 can be immobilized on various inert support materials, as implemented in fixed-film and fixed-bed reactors (Pozzo, Baltanás & Cassano, 1997; Braham & Harris, 2009; Manassero, Satuf & Alfano, 2017). A slurry reactor is characterized by a high-contact surface area, thus providing greater efficiency due to shorter reaction time and simple operation. This system requires a turbulent regime to ensure that the photocatalyst remain in suspension. However, TiO2 removal from the liquid phase after use is a very difficult task. Additionally, the fulfilment of these requirements increases substantially the energy consumption involved in the overall process of the water treatment. In recent years, the use of the photocatalyst supported (immobilized) by different materials, in different reactor configurations has shown to be a good strategy to circumvent these difficulties (Braham & Harris, 2009; Chong et al., 2010; Saleiro et al., 2010; Miranda-García et al., 2010; Spasiano et al., 2015; Amir, Julkapli & Hamid, 2017; Manassero, Satuf & Alfano, 2017; Srikanth et al., 2017).

One of the most widespread commercial catalysts for water/wastewater treatment is the TiO2 Aeroxide® P25 (TiO2-P25). This catalyst has shown good performance in degrading various persistent organic compounds found in aqueous matrices (Braham & Harris, 2009; Spasiano et al., 2015). The commercial TiO2-P25 is a powder mixture of rutile and anatase phases of TiO2 with the average particle size ranging from 35 to 65 nm and specific surface area of around 52 m2 g−1. The better photocatalytic efficiency of this material, as compared to pure rutile and anatase forms of TiO2, can be attributed to structural defects caused by the coexistence of anatase (80%) and rutile (20%) phases (Chong et al., 2010; Miranda-García et al., 2010; Pelaez et al., 2012).

In this context, the use of commercial TiO2-P25 immobilized on small glass spheres or beads resulted in significant improvement of the photocatalytic treatment. The mix TiO2 (sol–gel TiO2 and TiO2-P25) used for dip-coating immobilization on glass sphere resulted in good treatment performance for degrading emerging contaminants (Miranda-García et al., 2010; Miranda-García et al., 2014) and pesticides (Jiménez et al., 2015) in wastewater using a pilot Compound Parabolic Concentrator (CPC) type reactor. Heat attachment method for the immobilization of TiO2-P25 on glass beads was successfully applied to remove dyes (Khataee, 2009; Rasoulifard et al., 2014; Sheidaei & Behnajady, 2015a; Sheidaei & Behnajady, 2015b) and pharmaceuticals (Shankaraiah et al., 2016; Shargh & Behnajady, 2016a; Shargh & Behnajady, 2016b) with the use of UVC radiation instead of sunlight. When two different methods of TiO2 immobilization on glass beads (sol–gel and TiO2-P25 dispersed in water) were applied to remove Congo red dye, the photocatalytic degradation performed better with the second method (Qiu & Zheng, 2007).

The strength of the TiO2 coating adherence to a support is a relevant parameter for immobilized TiO2 photocatalysis and this characteristic has been widely investigated by different experimental approaches (Nakata & Fujishima, 2012; Srikanth et al., 2017). Leaching of immobilized TiO2 can be also used to assess the adherence strength of TiO2 coating. However, to our knowledge, leaching of the TiO2 immobilized on glass, so far has not been extensively investigated, which should be done, considering the diversity of immobilized methods that has been applied.

Deactivation and regeneration of the catalyst are relevant aspects to be taken into account when scaling up heterogeneous photocatalysis, due to the economic implications (Miranda-García et al., 2014). Adsorption and strong interaction between the active sites on the catalyst surface and the oxygen-bearing reaction intermediates leads to an abrupt decrease in the number of active sites during catalyst reaction (Prieto, Fermoso & Irusta, 2007). Several types of reactivation methods have been tested to regenerate deactivated photocatalysts, such as: the use of chemicals (HNO3, NaOH, NH4OH, H2O2 combined or not with UV irradiation) and water washing (Portela et al., 2007; Kanna et al., 2010; Miranda-García et al., 2014; Yanyan et al., 2017); UV exposure with pure air (Peral & Ollis, 1992); high humidity conditions (Jeong et al., 2013) for air pollution treatment; sonication treatment with water and methanol (Shang et al., 2002) and thermal processes (Cao et al., 2000; Miranda-García et al., 2014; Herrera, Reyes & Colina-Márquez, 2016; Odling et al., 2017).

Based on a recent review on supporting materials for immobilized photocatalytic applications in wastewater treatment (Srikanth et al., 2017), it was concluded that not only new studies focusing on photocatalytic activity under visible and/or solar light spectrum are required, but also recycled over many runs without significant loss in photocatalytic activity. Moreover, this review revealed that more investigations overcoming inherent limitations of immobilized catalysis are required, in order to make future scaling up feasible.

In this context, in the present investigation TiO2 was immobilized on glass spheres and evaluated regarding its performance in photocatalytic degradation using methylene blue (MB) as a model of pollutant. MB discoloration was performed in laboratory scale using a CPC type reactor, which has proven to be an efficient and widely applied reactor configuration in photocatalysis experiments (Tanveer & Guyer, 2013), under irradiation simulating the sunlight. A simple approach to catalyst’s immobilization on glass sphere is presented. It employed a suspended nanocrystaline TiO2-P25 powder in alcohol and acid medium, with the improved photocatalytic activity by polyethylene glycol (PEG) solution (Miranda-García et al., 2011; Nawawi et al., 2017). The leaching and regeneration capacity of the immobilized TiO2 were evaluated in specially designed tests.



Titanium dioxide Aeroxide® P25 (TiO2-P25) was purchased from Evonik, Brazil. Nitric acid (65%), ethanol and 2-propanol were supplied by Sigma-Aldrich (St. Louis, MO, USA) and Polyethylene glycol PEG-600 (MW: 560–640) by Merck (Darmstadt, Germany). MB was purchased from Cinética (Rio de Janeiro, Brazil). Aqueous solutions containing 10 ppm of MB was prepared with distilled water and used as model of wastewater in the photocatalytic experiments.

Immobilization of TiO2 on glass spheres

Borosilicate glass spheres (Ø = 5 mm) were coated with TiO2 film using the dip-coating process. Glass spheres were pre-treated in an ultrasonic bath (Unique, USC-1400A) during 60 min, using a solution of ethanol and distilled water (1:1). After that, the glass spheres were dried at 100 °C for 12 h. The coating of TiO2 on glass spheres was done according to methods previously described (Miranda-García et al., 2010; Manassero, Satuf & Alfano, 2017), with few modifications introduced in the present investigation. 6 g of TiO2-P25 was added to 150 mL of 2-propanol (being also possible to use ethanol), and the suspension was maintained in ultrasonic bath for 30 min. A volume of 30 µl of nitric acid was added to the suspension, and the obtained material was kept for 30 min in ultrasonic bath. A PEG 600 solution in 2-propanol was then added to reach a final concentration of 200 mg L−1, in order to provide a high porosity for the particles (Miranda-García et al., 2010; Miranda-García et al., 2014). This suspension was maintained another 30 min in the ultrasonic bath. After that, the glass spheres were coated by dip-coating with the modified oxide, holding them for 60 s in this suspension, being this process repeated twice. Finally, these glass spheres were dried at 80 °C for 90 min and calcined at 400 °C for 120 min, using a heating rate of 5 °C min−1.

In order to know the main properties of the TiO2 calcined at 400 °C, a control sample was prepared as follows. The TiO2 remained in suspension after the dip-coating process was recovered by solvent removal, using a rotary evaporator (IKA RV10). This material was then submitted to the same thermal treatment applied for the TiO2 supported on the glass spheres. The control sample of calcined TiO2 is identified hereafter as TiO2-400 °C.

Glass plates to assess titanium leaching in water

Before coating the glass spheres with TiO2, a leaching test was done with TiO2 supported on glass plates of borosilicate, the same material as the glass spheres. The deposition of TiO2-P25 on glass plates were carried out by a similar procedure as described in the previous section. The leaching test of TiO2-400 °C on glass plates consisted in the introduction of plates inside a beaker containing ultrapure water (Milliq®; Millipore, Hayward, CA, USA). The plates were kept under water agitation, using a shaker (Quimis, Cascavel, Paraná, Brazil) for 24 h. The amount of titanium leached in water was measured by ICP Optical Emission Spectrometry (OES) (700 series; Agilent Technologies, Santa Clara, CA, USA) in an accredited commercial laboratory (LabAgua, Rio de Janeiro, Brazil), according to the standard method 3120 B (APHA, 2012). All assays were conducted in triplicate.

In order to estimate the mass of the catalyst immobilized on the glass plates, a gravimetric analysis was used. The plates were weighed after moisture removal (110 °C for 1 h), before and after exposure in ultrapure water for 24 h. Then, they were immersed in a 10% solution of nitric acid and maintained under ultrasonic bath for 1 h to remove TiO2 film. The plates were then washed and dried (110 °C for 1 h) and weighed again. The leached ratio (LR) of Ti was calculated as following (Eq. (1)): L R % = W l W m × 100 where: Wl is the leached mass of Ti measured by ICP-OES in water, and Wm is the initial mass of TiO2 immobilized on glass plates.

Materials characterization

The powder samples of TiO2-P25 and TiO2-400 °C were characterized by X-ray powder diffraction (XRD) and Brunauer–Emmett–Teller (BET) N2 adsorption. In addition, TiO2 immobilized on glass spheres images were collected using scanning electron microscopy (SEM). These techniques are briefly described below.


X-ray powder diffraction (XRD) patterns of the samples were obtained with a Brüker D8 Focus diffractometer in the Bragg-Brentano geometry, using Cu K-alpha radiation and a secondary graphite crystal monochromator. The diffraction patterns were collected over a 2Θ range of 10°–80° at a step of 0.02° 2Θ and acquisition time of 20 s per step with scintillation detector. The phase composition determination and the estimation of mean crystallite size were performed employing the Topas-Academic software. Instrument function was obtained at the same instrumental configuration using NIST standard reference material SRM1976 (α-Al2O3).

The Rietveld method of powder diffraction pattern fitting and structural (microstructural) refinement by convolution approach to peaks profile modeling implemented in the Topas-Academic software was used to obtain the crystalline phase composition and the average crystallite sizes of the respective phases. The Voigt function was employed to model the crystallites size effect, which consists in a characteristic broadening of X-ray diffraction peaks. Isotropic model of size broadening which implies a spherical shape of crystallites well described the diffraction peak profiles. A sample average volume weighted thicknesses of crystallites defined by the Stokes’ and Wilson’s equation (Stokes & Wilson, 1942) were calculated using Eq. (2): L V = λ β cos θ where: β is the integral breadth of the diffraction line (peak area divided by peak maximum), λ is the wavelength of the X-rays and θ is the half of the diffraction angle.


The TiO2 coated glass spheres were examined by scanning electron microscopy (SEM) in order to characterize the surface morphology of the TiO2 films and aggregates, including the eventual formation of large-sized TiO2 agglomerations that can lead to cracks formation, which can lead to detrimental effects on long-term mechanical stability of the coating in applications involving water matrix. SEM images of TiO2-coated glass spheres, before and after photocatalysis experiments were acquired using a Helios Nanolab 650 Dual Beam. The SEM images were obtained using 2 kV, 13 pA, FEG filament and using ETD and TLD detectors. Samples were dropped in carbon conductive adhesive tapes.


For the determination measurements of the specific surface area and total pore volume, Brunauer–Emmett–Teller (BET) N2 adsorption were carried out using a Autosorb-1 analyzer (Quantachrome Instruments, Boynton Beach, FL, USA) automated apparatus using liquid N2 adsorption at a temperature of 140 °C. Specific surface area was determined in the relative pressure range between 0.05 and 0.3.

Photodegradation tests

CPC reactor

The evaluation of the photocatalytic and adsorption capability of the TiO2-400 °C catalyst immobilized on glass spheres was done with a lab scale compound parabolic collector reactor (CPC), using an Ultra-vitaluz OSRAM 300W lamp, that simulates the solar spectrum (Heredia, Sham & Farfán-Torres, 2015). The average irradiance was adjusted around 30 Wm−2 of UVA-light intensity, using a Delta Ohm model HD-2302 radiometer. The reactor was built using a borosilicate glass tube (external diameter of 30 mm, wall thickness of 2.0 mm, and length of 200 mm) and a polished anodized aluminum surface, made in the form of an involute, used as reflector (Fig. 1) (Rodríguez et al., 2004; Duarte et al., 2005). The schematic drawing of photodegradation experiments is presented in Fig. S1, Appendix S1.

Glass spheres coated with TiO2-400 °C, filling borosilicate tubes in the CPC reactor.
Figure 1: Glass spheres coated with TiO2-400 °C, filling borosilicate tubes in the CPC reactor.

The flow rate used in all experiments was 500 mL min−1. A peristaltic pump (Watson-Marlon 502S) and a magnetic stirrer were used to recirculate and homogenize the 500 mL of the 10 ppm MB-containing solution. The temperature and pH of the solution varied, respectively, from 25 °C to 30 °C and from 6.3 to 6.7 throughout the experiment. Samples of the solution (4 mL) were collected during the experiment, being the absorbance measured at 664 nm using a HACH DR 5000 UV-Vis spectrophotometer. Five treatment cycles were applied with the same photocatalyst. The solution was recirculated under dark condition for 30 min to ensure adsorption–desorption equilibrium before illumination (Miranda-García et al., 2010; Zhang et al., 2015), only for the first cycle. To regenerate the catalyst, before the fifth cycle, distilled water was recirculated, under irradiation, into the reactor during 180 min. The efficiency of MB removal solution was calculated according to Eq. (3): E = 1 C n C o × 100 where: Cn is the MB concentration at a time t from the beginning of the recirculation test and Co is the initial MB concentration.

The pseudo first-order apparent rate constant (k, min−1) related to the discoloration of MB, an approximate measure of the photocatalytic activity (Borges et al., 2016) was determined from the regression curve ln(Cn/Co) vs. irradiation time (França et al., 2016).

Results and Discussion

Materials characterization

Figure 2 shows the selected SEM images of the surface of the catalyst on glass spheres, before the photocatalytic treatment (A and C) and after five cycles of treatment (B and D).

SEM images of TiO2-400 °C on glass spheres surface before use (A and C) and after five photocatalytic treatment cycles (B and D).

Figure 2: SEM images of TiO2-400 °C on glass spheres surface before use (A and C) and after five photocatalytic treatment cycles (B and D).

The rough surface morphology of TiO2-400 °C films and presence of agglomerates composed of TiO2 nanoparticles, observed in the present study seems to be similar to the reported by other researchers (Chen & Dionysiou, 2006; Miranda-García et al., 2010; Khalilian et al., 2015). The SEM images (Fig. 2) also confirm that the morphology of the immobilized TiO2-400 °C remains mostly unchanged after several cycles of photocatalytic experiments, suggesting that the deposition of TiO2 over the glass spheres was efficient and a stable support was achieved.

Micro-structural characterization of TiO2 samples

The XRD patterns of the TiO2-P25 and TiO2-400 °C nanopowders are shown in Fig. 3. As expected, a two-phase material composed of anatase and rutile is perfectly in accordance with the standards observed in the X-ray diffraction samples. The main microstructural parameters of both samples, calculated from Rietveld refinement (crystalline phase composition and crystallite size, Lv) are shown in Table 1.

X-ray diffraction patterns of TiO2-P25 and TiO2-400 °C.

Figure 3: X-ray diffraction patterns of TiO2-P25 and TiO2-400 °C.

As one can see from Table 1, the thermal treatment of TiO2-P25 did not produce any substantial changes in the measured microstructural characteristics. Both, phase composition and average crystallite size, remained unaltered within the statistical errors of data modelling. This is confirmed by BET measurements. Figure 4 shows the nitrogen adsorption isotherms for TiO2-P25 and TiO2-400 °C. Type II adsorption isotherms were obtained, indicating a macroporous nature of the adsorbent with strong adsorbate-adsorbent interactions (Buddee et al., 2014).

Table 1:
Microstructural properties of TiO2-P25 and TiO2-400 °C.
Material Phase content (%) Crystalline size, Lv (nm) SBET Pore volume
Anatase Rutile Anatase Rutile (m2 g−1) (cm3 g−1)
TiO2-P25 86(1) 14(1) 20.5(8) 31(6) 56.2 0.129
TiO2-400 °C 87(1) 13(1) 21.1(8) 30(6) 53.9 0.137
DOI: 10.7717/peerj.4464/table-1
Nitrogen adsorption isotherms of the TiO2-P25 powder before and after calcination at 400 °C (TiO2-400 °C).

Figure 4: Nitrogen adsorption isotherms of the TiO2-P25 powder before and after calcination at 400 °C (TiO2-400 °C).

The specific surface area and the total pore volume of TiO2-P25, Table 1 do not change significantly after calcination. Nevertheless, a small reduction of the specific surface area and a small increase in the pore volume can be indicative of the formation of slightly larger or/and more regularly shaped (more spherical) TiO2 particles. This trend in the behaviour of the above mentioned properties of nanocrystaline TiO2 powders, due to an increase in the calcination temperature, has been reported in previous studies (Chen & Dionysiou, 2007; Viswanathan & Raj, 2009; Wang et al., 2012). These changes can be attributed to defects induced by the temperature annealing and coalescence of the crystallites. However, the character and the extent of the overall changes in the microstructural features corroborate with a limitation in the annealing processes in near-surface regions of the TiO2 particles. Consequently, the expected photocatalytic activity of the TiO2-400 °C immobilized on glass spheres is very similar to that of TiO2-P25.

Adherence of the TiO2 catalyst on glass plates

The adherence strength of the TiO2-400 °C immobilized on glass plates was evaluated by exposing the photocatalyst coating to stirring in ultrapure water (Milliq) for 24 h and subsequent measurement of the amount of TiO2 leached into the water. The assay was conducted in triplicates together with negative control samples (a blank using a glass plate). No visually detectable depletion of TiO2-400 °C coating on glass plates was observed after the treatment. The measured average TiO2 concentration in water after stirring the TiO2-400 °C coated on glass plates was 2.7 (±1.0) µg L−1. No TiO2 was detected in the water after stirring the negative control plate. The catalyst mass deposited on each plate was estimated as being equal to 16.6 (±1.9) mg L−1. The LR value was obtained to be 0.03% of TiO2 leached in water after 24 h. This LR value can be considered small when compared with data reported in other studies. For example, the LR of the TiO2 immobilized on glass plates was found to be (1.52 ± 0.12%) after 10 h of stirring treatment (Nawi et al., 2011), while in a recent study (Lam et al., 2017) approximately 10% of the TiO2 immobilized on glass beads was leached into water. In addition it was reported (Jawad et al., 2016) that 7.3% of the TiO2 of a TiO2/epoxidized natural rubber (ENR) immobilized on glass plates was leached after 4 h.

Methylene Blue (MB) degradation

To confirm the photocatalytic activity of the TiO2-400 °C immobilized on glass spheres as produced in the present investigation, the degradation of MB, used as a model of oxidizable substrate, expressed in terms of its discoloration, was evaluated.

At the beginning, the glass spheres were inserted in the reactor and washed several times with distilled water to eliminate non-bonded or weakly bonded TiO2 and to avoid any effect produced by suspended TiO2 nanoparticles, eventually released from the immobilized photocatalyst.

In a typical experimental cycle, around 1,500 spheres (Ø = 5 mm) coated by the photocatalyst (around 0.3 ± 0.1 mg of TiO2 immobilized per sphere) were placed into the glass tube of the CPC reactor. The thickness of the TiO2-400 °C layer on glass spheres was estimated as a function of the mass in each sphere (about 0.3 mg), density and total layer volume (glass sphere volume plus TiO2 layer). For calculation purpose, the TiO2 layer considered uniform and a cubic equation was used. The value obtained was about 1 µm. This value was considered reasonable in comparison to previous studies (Negishi et al., 2007; Espino-Estévez et al., 2015).

As reported before, the MB degradation was carried out for 90 min using an artificial lamp that simulates the solar spectrum in the CPC reactor. Before the photocatalytic experiments, the level of adsorption of MB on the photocatalyst was evaluated in experiments involving the recirculation of the solution in the absence of light, and the MB degradation by photolysis was assessed, using the same lamp as irradiation font. In order to evaluate other possible MB adsorption processes in the CPC reactor, the solution containing MB was recirculated under similar experimental conditions, but without the presence of catalyst and light. Figure 5 shows the results of the MB degradation mediated by TiO2-400 °C supported on glass spheres, together with the non-catalytic photolysis and MB adsorption (without catalyst nor irradiation), carried out in the CPC system.

Methylene blue (MB) adsorption in the CPC reactor (without catalyst and light) and its degradation (measured as discoloration %) by photolysis and photocatalytic using glass spheres coated by TiO2-400 °C.

Figure 5: Methylene blue (MB) adsorption in the CPC reactor (without catalyst and light) and its degradation (measured as discoloration %) by photolysis and photocatalytic using glass spheres coated by TiO2-400 °C.

As shows in Fig. 5, in the first cycle with TiO2 glass spheres the colour given by MB was almost completely removed (96%) in 90 min of photocatalytic reaction and that only 19% of the initial colour disappeared due to photolysis. It was also observed that the adsorption of MB in the catalyst is minimal around the rated range. This result confirms those obtained in previous investigations (Munjal, Dwivedi & Bhaskarwar, 2015; Cha et al., 2017). For this reason, the adsorption of the immobilized material during subsequent cycles was considered negligible.

The remaining photocatalytic capacity of used material was checked, following a series of five photocatalytic cycles. Before running the last cycle, distilled water was recirculated into the CPC reactor containing the glass spheres coated with TiO2-400 °C, under irradiation during 180 min. The levels of discoloration after 90 min of reaction, in terms of percentage and their respective pseudo-first order kinetics constants are shown, respectively, in Fig. 6 and Table 2.

Evolution of methylene blue (MB) discoloration (%) with the number of cycles.

Figure 6: Evolution of methylene blue (MB) discoloration (%) with the number of cycles.

Table 2:
Pseudo first order kinetics constant k (min−1) for MB discoloration in each cycle (±standard error).
Cycle 1 Cycle 2 Cycle 3 Cycle 4 Cycle 5
k 0.036 (0.00062) 0.030 (0.00028) 0.025 (0.00028) 0.020 (0.00005) 0.039 (0.002)
DOI: 10.7717/peerj.4464/table-2

As shown in Fig. 6, the degradation efficiency using TiO2-400 °C supported on glass spheres suffered a gradual decrease with repeated use. The photocatalytic activity was recovered after the fourth cycle with the washing of the catalyst under solar radiation simulated for 180 min, which can be viewed on the fifth cycle of degradation. The observed deactivation of the catalyst should be due to strong interactions between the active sites on the catalyst surface and the dye, as well as to the dye adsorption, leading to loss of function of part of the active sites of the catalyst. The blue color characteristic of MB found in the glass spheres containing the catalyst observed after each cycle of the photocatalytic treatment supports this hypothesis. A similar effect has been reported previously (Kanna et al., 2010; Salehi, Hashemipour & Mirzaee, 2012).

The pseudo first order kinetics constants (Table 2) corroborates the statements above, since the kinetics constants decreases in sequence after each cycle of treatment, unless for the last cycle, which used the catalyst after its regeneration.

In a recent investigation, after 180 min of irradiation about 10 and 90% of the MB in solution (10 mg L−1) was degraded using respectively, TiO2 and N-doped TiO2 immobilized on glass bead (Kassahun et al., 2017). Compared to those results, the immobilized TiO2-400 °C photocatalyst used in the present investigation represents a breakthrough in the knowledge, since in our study it was possible to degrade in 90 min more than 90% of the initial concentration of the same dye (MB). Moreover, the present investigation reached an effective regeneration of photocatalytic activity applied to MB removal, using only distillate water and simulated solar radiation by lamp (UV-vis light), which is a simple and non-expensive approach to efficiency recovery of material.


The present investigation describes a simple procedure to obtain an efficient TiO2-based photocatalyst immobilized through a very stable coating and with good adhesion on borosilicate glass spheres. SEM microscopy, XRD and BET showed that microstructural features of TiO2-P25 remained almost unaltered after calcination at 400 °C. Generally, the main limitation of immobilization of photocatalysts is not only in the loss of photocatalytic activity, but also due the decrease of the coating integrity during its use. This is not the case of the material presented in this study, since the photocatalyst immobilization did not compromise its activity, and the adhesion on glass spheres proved to be quite effective even after exhaustive leaching tests in water.

Under simulated solar irradiation at conservative power (30 W m−2 within the UVA range), using a lab scale CPC reactor, the immobilized TiO2-400 °C photocatalyst could degrade up to 96% of the MB present in aqueous solutions in 90 min of reaction. The reuse of the photocatalyst resulted in a decrease of its photocatalytic activity due to the adsorption of MB in active sites of the catalyst, which could be reversed by washing with water, under simulated solar irradiation for 180 min. This result confirms the effective regeneration of the photocatalyst by a simple and non-expensive approach. In addition, the immobilized TiO2-400 °C on glass spheres obtained through the procedure described in the present study is a promising indication of its applicability to environmental remediation and wastewater/water treatment based on heterogeneous photocatalysis.

Supplemental Information

Schematic drawing of photodegradation experiments

(1) beaker; (2) magnetic stirrer; (3) peristaltic pump; (4) CPC reactor (collector and borosilicate glass tube); and (5) solar spectrum simulated lamp.

DOI: 10.7717/peerj.4464/supp-1
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