Semiconductor-Based Photocatalytic, Photoelectrochemical, and Photovoltaic Solar-Energy ConversionView this Special Issue
Research Article | Open Access
Chin Wei Lai, "Photocatalysis and Photoelectrochemical Properties of Tungsten Trioxide Nanostructured Films", The Scientific World Journal, vol. 2014, Article ID 843587, 7 pages, 2014. https://doi.org/10.1155/2014/843587
Photocatalysis and Photoelectrochemical Properties of Tungsten Trioxide Nanostructured Films
Tungsten trioxide (WO3) possesses a small band gap energy of 2.4–2.8 eV and is responsive to both ultraviolet and visible light irradiation including strong absorption of the solar spectrum and stable physicochemical properties. Thus, controlled growth of one-dimensional (1D) WO3 nanotubular structures with desired length, diameter, and wall thickness has gained significant interest. In the present study, 1D WO3 nanotubes were successfully synthesized via electrochemical anodization of tungsten (W) foil in an electrolyte composed of 1 M of sodium sulphate (Na2SO4) and ammonium fluoride (NH4F). The influence of NH4F content on the formation mechanism of anodic WO3 nanotubular structure was investigated in detail. An optimization of fluoride ions played a critical role in controlling the chemical dissolution reaction in the interface of W/WO3. Based on the results obtained, a minimum of 0.7 wt% of NH4F content was required for completing transformation from W foil to WO3 nanotubular structure with an average diameter of 85 nm and length of 250 nm within 15 min of anodization time. In this case, high aspect ratio of WO3 nanotubular structure is preferred because larger active surface area will be provided for better photocatalytic and photoelectrochemical (PEC) reactions.
Design and controlled growth of nanostructure semiconductor assemblies has gained significant attention in recent years due to the scientific interests and potential applications [1, 2]. In this manner, WO3 is one of the famous electrochromic inorganic materials since Deb’s discovery in 1969 . WO3 film exhibits a broad range of functional properties, such as small band gap energy (2.4–2.8 eV), deeper valence band (+3.1 eV), stable physicochemical properties, and strong photocorrosion stability in aqueous solution [4–10]. The characteristics of WO3 film make them suitable for electrochromic layers in a smart window . Many studies pertaining to WO3 nanostructures are mainly aimed at the formation of high active surface area in view of their use in electrochromic applications [9, 10]. However, several studies have reported that growth of well-aligned and uniformity of anodic WO3 nanotubular structure was a difficult task and most of the studies were only able to grow anodic WO3 into nanoporous instead of nanotubular structure [7–10, 12, 13]. In the present study, we describe the synthesis of well-aligned anodic WO3 nanotubes using electrochemical anodization technique in a fluorinated-based electrolyte. To the best of our knowledge, literatures on optimization of the geometrical features of regular anodic WO3 nanotubular structures are still lacking. Thus, such mechanistic studies and understanding are very important to tailor the desired length, pore size, and wall thickness of ordered WO3 nanotubular structures for high surface area to volume ratio. In this study, a comprehensive experiment was conducted to control the one-dimensional nanostructure of anodic WO3 using electrochemical anodization to achieve effective photocatalytic degradation of MO dye and H2 gas generation via PEC water splitting process.
2. Experimental Procedure
The high purity (99.95% purity with 0.1 mm in thickness) tungsten (W) foils from Alfa Aesar USA were used in this study. Prior to anodization, W foils were degreased in ultrasonic bath containing ethanol for 30 minutes. The foils were then rinsed in deionized water and dried in nitrogen stream. Then, anodization was performed in a two-electrode configuration bath with W foil served as the anode and the platinum electrode served as the counter electrode. The electrolyte is composed of 100 mL of 1 M of sodium sulfate (Na2SO4, Merck, USA) solution with ammonium fluoride (NH4F, Merck, USA) at 40 V with sweep rate of 1 V/s. In the present study, different content of NH4F (0.3, 0.5, and 0.7 wt%) will be added into 1 M Na2SO4 solution for several anodization duration (15, 30, and 60 min) in order to investigate the formation of anodic WO3 nanotubular structures. As-anodized anodic WO3 samples were cleaned using acetone (J.T. Baker, Nederland) and dried in nitrogen stream after anodization process. The morphologies of anodic WO3 nanostructures were observed by field emission scanning electron microscopy (FESEM), using a FEI Quanta 200 (FESEM model, USA) at a working distance of around 1 mm. The cross-sectional observation was carried out on mechanically bent samples to get the thickness of the oxide layer. The chemical stoichiometry of the sample was characterized using energy dispersive X-ray (EDX) analysis, which is equipped in the FESEM. In order to assess the photocatalytic performance of the anodic WO3 nanostructure formed, anodized W foil of 25 mm × 25 mm was prepared and placed in 200 mL of 30 ppm MO dye in a customized photoreactor made of quartz glass. Two different surface morphologies of anodic WO3 nanostructure were selected for MO dye degradation purpose (e.g., oxide layer and nanotubular structure). In the present study, both samples were left in the photoreactor for 30 min in a dark environment to achieve adsorption/desorption equilibrium. Then, both samples were photo-irradiated at room temperature by using a 150 W Xenon solar simulator (Zolix LSP-X150) with intensity of 800 W/m2. A 5 mL solution was removed at an interval of 1 h from the photoreactor, and concentration of the solution was measured using a UV spectrophotometer (PerkinElmer Lambda 35). Next, the photoelectrochemical properties of the selected samples were further characterized using a three-electrode water splitting cell, with WO3 nanotubes as the working electrode, platinum rod as the counter electrode, and saturated calomel electrode (SCE) as the reference electrode. The bath with electrolyte composed of 0.5 M sulfuric acid aqueous solution was selected in this experimental work. The H2 gas generated at platinum rod was collected using the water displacement technique. As the H2 gas was produced in counter electrode in water splitting chamber, it was bubbling up into inverted burette. The volume of H2 gas was determined by reading the gas level on the side of burette.
3. Results and Discussion
In the present study, the effect of fluoride content and anodization time on the morphology of anodic WO3 layer was investigated. Figure 1 to Figure 3 showed the surface morphologies of anodic WO3 layer in different fluoride content electrolyte from 15 min up to 60 min of anodization time. As shown from the FESEM images, the appearance of anodic WO3 layer was strongly dependent on the fluoride content and anodization times. Then, the EDX analysis was employed to investigate the composition of element of W and O from the anodic WO3 layer. Based on the results obtained, the atomic percentage of W element was about 55 at% and O element was about 45% at%. During electrochemical anodization, fluoride content played an important role in controlling the chemical dissolution rate at the interface of W/WO3 . Figure 1 exhibited variations of WO3 surface morphology under low 0.3 wt% fluoride content electrolyte for different anodization times. It could be observed that formation of oxide layer on W foil was incomplete at 15 min of anodization time (Figure 1(a)). Interestingly, only thin compact oxide layer with randomly pits was formed after prolonging the anodization time to 30 min and 60 min (Figures 1(b) and 1(c)). The resultant thickness of oxide layer was approximately 100 nm. These results indicated that low fluoride concentration was insufficient in forming the deep and large pore size on the oxide layer due to the inactive chemical dissolution reaction . In this case, oxygen ions within the electrolyte through the W surface towards the W/WO3 interface induce further growth of the oxide layer under applied potential. The high electric field across the oxide layer of WO3 and subsequently induce the polarization of W–O bonding, which is able to transfer the W6+ ions from the pores and leave behind random pits [14, 15]. By further increasing the content of fluoride to 0.5 wt%, the irregular anodic WO3 nanoporous structure with thickness of approximately 200 nm could be observed from Figures 2(a) to 2(c). However, it could be noticed that the pore diameter on the oxide layer was increasing up to 70 nm when prolonging the anodization time to 60 min. The uniform anodic nanoporous WO3 layer could be achieved in 1 M Na2SO4 electrolyte composed of 0.5 wt% fluorides content. When the fluoride content was further increased to 0.7 wt%, a hollow cylinder oxide nanostructure was observed as shown in Figure 3(a), which indicated that the amount of fluoride in the electrolyte was sufficient to increase the chemical dissolution rate. This condition led to further acidification reactions to develop the nanoporous structure into nanotubular structure [16–18]. In this case, tungsten fluoro-complex ions within the electrolyte playing an important role in inducing chemical dissolution to enlarge and deepen pores and eventually transforming to nanotubular structure . It is noteworthy to mention that the WO3 nanotubes with diameters of approximately 85 nm and lengths of 250 nm were successfully formed when the fluoride content was increased to 0.7 wt%. However, nanotubular structure disappeared when further the anodization time increased to 30 min and 60 min and eventually resulted in irregular nanoporous structure (Figures 3(b) and 3(c)). The reason might be attributed to the excessive chemical etching on the wall surface of nanotubes during the chemical dissolution reactions. Thus, optimization of fluoride content identified in our electrolyte was 0.5 wt% in order to grow the well-aligned one-dimensional WO3 nanotubes for 15 min electrochemical anodization duration. Figure 4 presented a simple schematic illustration of formation of anodic WO3 nanostructured film during electrochemical anodization stage in the presence of insufficient and adequate fluoride content.
The photocatalytic removal ability of the selected sample of anodic WO3 oxide layer was compared with that of the anodic WO3 nanotubular structure by exposing the samples to MO dye under solar illumination. The initial MO dye concentration in the solution was fixed at 30 ppm. The changes in MO dye concentration were investigated within 5 hours and the result was shown in Figure 5. The degradation rates of MO dye concentration for sample “anodic WO3 oxide layer” and sample “anodic WO3 nanotubular structure” was decreased from 30 ppm to 13.5 ppm and 8.5 ppm, respectively. When anodic WO3 nanotubular structure exposed to the hv illumination that solar photonic energy is higher than its band gap energy (2.4–2.8 eV), the anodic WO3 itself will generate pairs of photo-induced electrons (e−) and holes (h+). In this manner, the e− and oxygen molecule (O2) will combine to form super oxide anion (), whereas the h+ of anodic WO3 and water molecule (H2O) will generate hydroxyl radical (•OH). These powerful oxidizing agents (•OH and ) will then decompose the MO dye (organic dye) into CO2 and H2O. This cycle will continue when the hv illumination is available. A simple schematic illustration of basic principal in photocatalytic degradation of MO dye is shown in Figure 6. In theoretical perspectives, the photocatalytic degradation performance of anodic WO3 can be related on the ability to generate pairs of charge carriers, which will release powerful oxidizing agents (•OH and ) that are able to undergo the secondary reactions. In other words, anodic WO3 nanotubular structure with larger surface area of active reaction sites (inner and outer wall surface of nanotubes) has better photon absorption under hv illumination. The distance of light scattering inside the nanotubes extends and provides more photon absorption to trigger the photocatalytic degradation reaction.
On the other hand, the evolution rate of H2 gas generated from the photoelectrochemical (PEC) water-splitting process under solar illumination was measured. The H2 evolution as a function of time is shown in Figure 7. H2 generation rate from water splitting reaction increased linearly with increasing exposure time. The sample (anodic WO3 nanotubular structure) achieved a maximum evolution of approximately 1 mL/cm2 within 1 hour, which is relatively higher compared with the anodic WO3 oxide layer. The H2 production completely stopped after the termination of hv illumination. This observation clearly shows that H2 is only produced photocatalytically. A constant production rate of H2 gas could be observed in the present study. In theoretical perspectives, PEC water splitting process is the general term for a chemical reaction in which water is separated into O2 and H2 using anodic WO3 film that catalyze the water splitting reaction. A basic schematic diagram of such overall water splitting reaction using a semiconductor photocatalyst is presented in Figure 8. The water splitting reaction can be summarized as follows: 2H2O(l) → O2(g) + 2H2(g). The overall water splitting reaction is considered as a thermodynamically uphill reaction with a large Gibbs free energy of KJ mol−1. This reaction indicates that photon energy is required to overcome the large positive change in Gibbs free energy through PEC water splitting process [19, 20]. The light-driven water splitting process is triggered when anodic WO3 film absorbs photons from hv illumination with energies greater than its band gap energy. This light absorption generates negative e− in the conduction band and positive h+ in the valence band. The h+ performs work at the anodic WO3 electrolyte interface oxidizing water molecules to create O2 and H+ ions within the electrolyte. Then, the e− will move through the external circuit to the platinum electrode (counter electrode) where they reduce H+ ions creating H2 molecules due to the electric field or under external bias . The PEC water splitting performance is consistent with the photocatalytic degradation. In summary, the self-organized WO3 nanotubular structure has strong ability to release much more photo-induced e−/h+ pairs than that of compact layer structure. Thus, it is crucial to maximize the active surface area of photocatalyst (anodic WO3) for better photocatalytic and photoelectrochemical performance.
In conclusion, complete transformation of W foil to one-dimensional WO3 nanotubes with an average diameter of 85 nm and length of 250 nm could be achieved within 15 min in an electrolyte composed of 1 M of Na2SO4 and 0.7 wt% of NH4F. The main reason attributed to the sufficiency of tungsten fluoro-complex ions induced chemical dissolution to enlarge and deepen pores and eventually transform to nanotubes. The ability to grow large active surface area of anodic WO3 nanostructures demonstrated a substantial enhancement in the degradation of MO dye and H2 generation via water splitting process, as compared to the anodic WO3 oxide layers.
Conflict of Interests
The author declares that there is no conflict of interests regarding the publication of this paper.
This research is supported by High Impact Research Chancellory Grant UM.C/625/1/HIR/228 (J55001-73873) from the University of Malaya. In addition, authors would like to thank University of Malaya for sponsoring this work under University of Malaya Research Grant (UMRG, RP022-2012D).
- C. A. Grimes, “Synthesis and application of highly ordered arrays of TiO2 nanotubes,” Journal of Materials Chemistry, vol. 17, pp. 1451–1457, 2013.
- C. W. Lai and S. Sreekantan, “Preparation of hybrid WO3-TiO2 nanotube photoelectrodes using anodization and wet impregnation: improved water-splitting hydrogen generation performance,” International Journal of Hydrogen Energy, vol. 38, no. 5, pp. 2156–2166, 2013.
- S. K. Deb, “A novel electrophotographic system,” Applied Optics, vol. 8, no. 1, pp. 192–195, 1969.
- C. Trimble, M. DeVries, J. S. Hale, D. W. Thompson, T. E. Tiwald, and J. A. Woollam, “Infrared emittance modulation devices using electrochromic crystalline tungsten oxide, polymer conductor, and nickel oxide,” Thin Solid Films, vol. 355, pp. 26–34, 1999.
- I. Bedja, S. Hotchandani, R. Carpentier, K. Vinodgopal, and P. V. Kamat, “Electrochromic and photoelectrochemical behavior of thin WO3 films prepared from quantized colloidal particles,” Thin Solid Films, vol. 247, no. 2, pp. 195–200, 1994.
- C. W. Lai and S. Sreekantan, “Fabrication of WO3 nanostructures by anodization method for visible-light driven water splitting and photodegradation of methyl orange,” Materials Science in Semiconductor Processing, vol. 16, no. 2, pp. 303–310, 2012.
- A. Watcharenwong, W. Chanmanee, N. R. de Tacconi, C. R. Chenthamarakshan, P. Kajitvichyanukul, and K. Rajeshwar, “Anodic growth of nanoporous WO3 films: morphology, photoelectrochemical response and photocatalytic activity for methylene blue and hexavalent chrome conversion,” Journal of Electroanalytical Chemistry, vol. 612, no. 1, pp. 112–120, 2008.
- X. Zhang, K. Huo, L. Huo, L. Hu, and P. K. Chu, “Fabrication and photocatalytic activity of nanoporous WO3 film,” Nanoscience and Nanotechnology Letters, vol. 2, no. 1, pp. 51–57, 2010.
- W. Li, J. Li, X. Wang, S. Luo, J. Xiao, and Q. Chen, “Visible light photoelectrochemical responsiveness of self-organized nanoporous WO3 films,” Electrochimica Acta, vol. 56, no. 1, pp. 620–625, 2010.
- S. Berger, H. Tsuchiya, A. Ghicov, and P. Schmuki, “High photocurrent conversion efficiency in self-organized porous WO3,” Applied Physics Letters, vol. 88, no. 20, Article ID 203119, 2006.
- C. G. Granqvist, “Electrochromic tungsten oxide films: review of progress 1993–1998,” Solar Energy Materials and Solar Cells, vol. 60, no. 3, pp. 201–262, 2000.
- V. Cristino, S. Caramori, R. Argazzi, L. Meda, G. L. Marra, and C. A. Bignozzi, “Efficient photoelectrochemical water splitting by anodically grown WO3 electrodes,” Langmuir, vol. 27, no. 11, pp. 7276–7284, 2011.
- Y. Nah, A. Ghicov, D. Kim, and P. Schmuki, “Enhanced electrochromic properties of self-organized nanoporous WO3,” Electrochemistry Communications, vol. 10, no. 11, pp. 1777–1780, 2008.
- C. W. Lai, S. B. A. Hamid, and S. Sreekantan, “A novel solar driven photocatalyst: well-aligned anodic WO3 nanotubes,” International Journal of Photoenergy, vol. 2013, Article ID 745301, 6 pages, 2013.
- C. W. Lai, S. Sreekantan, and Z. Lockman, “Photoelectrochemical behaviour of uniform growth TiO2 nanotubes via bubble blowing synthesised in ethylene glycol with hydrogen peroxide,” Journal of Nanoscience and Nanotechnology, vol. 12, no. 5, pp. 4057–4066, 2012.
- C. W. Lai, S. Sreekantan, and J. Nanomater, “Effect of applied potential on the formation of self-organized TiO2 nanotube arrays and its photoelectrochemical response,” Journal of Nanomaterials, vol. 2011, Article ID 142463, 7 pages, 2011.
- Y. C. Nah, I. Paramasivam, and P. Schmuki, “Doped TiO2 and TiO2 nanotubes: synthesis and applications,” ChemPhysChem, vol. 11, no. 13, pp. 2698–2713, 2010.
- Z. Su and W. Zhou, “Formation, morphology control and applications of anodic TiO2 nanotube arrays,” Journal of Materials Chemistry, vol. 21, pp. 8955–8970, 2011.
- D. Y. C. Leung, X. L. Fu, C. F. Wang et al., “Hydrogen production over titania-based photocatalysts,” ChemSusChem, vol. 3, no. 6, pp. 681–694, 2010.
- C. W. Lai and S. Sreekantan, “Study of WO3 incorporated C-TiO2 nanotubes for efficient visible light driven water splitting performance,” Journal of Alloys and Compounds, vol. 547, pp. 43–50, 2013.
Copyright © 2014 Chin Wei Lai. 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.