- About this Journal ·
- Abstracting and Indexing ·
- Aims and Scope ·
- Annual Issues ·
- Article Processing Charges ·
- Articles in Press ·
- Author Guidelines ·
- Bibliographic Information ·
- Citations to this Journal ·
- Contact Information ·
- Editorial Board ·
- Editorial Workflow ·
- Free eTOC Alerts ·
- Publication Ethics ·
- Reviewers Acknowledgment ·
- Submit a Manuscript ·
- Subscription Information ·
- Table of Contents
International Journal of Photoenergy
Volume 2013 (2013), Article ID 419182, 5 pages
H2 Fuels from Photocatalytic Splitting of Seawater Affected by Nano-TiO2 Promoted with CuO and NiO
1Department of Environmental Engineering, National Cheng Kung University, Tainan 70101, Taiwan
2Sustainable Environment Research Center, National Cheng Kung University, Tainan 70101, Taiwan
3Center for Micro/Nano Science and Technology, National Cheng Kung University, Tainan 70101, Taiwan
4Department of Environmental Science and Engineering, Tunghai University, Taichung 40704, Taiwan
5Department of Engineering and System Science, National Tsing Hua University, Hsinchu 30013, Taiwan
Received 30 May 2013; Revised 24 July 2013; Accepted 24 July 2013
Academic Editor: Jiaguo Yu
Copyright © 2013 A.-J. Simamora et al. 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.
To enhance H2 yields from the photocatalytic splitting of seawater, better photocatalysts such as nanostructured TiO2 promoted with NiO (2.5%) and CuO (2.5%) have been studied in the present work. The accumulated H2 yielded from the photocatalytic splitting of seawater containing oxalic acid (50 mM) as the sacrificial reagents on CuO/nano-TiO2 is 8.53 μmol/gcat after the 5 h radiation. On the NiO/nano-TiO2 photocatalyst, the H2 yield is relatively low (i.e., 1.46 μmol/gcat). Note that the hole scavenging with chlorides in seawater may be associated with the less H2 yielded from the seawater photocatalysis (on CuO/nano-TiO2) if compared with that from water (42.4 μmol/gcat).
Utilization of fossil energy which may cause air pollution or global warming has negative impacts on the human health and environment. Today’s world is also facing an urgency need in developing alternative fuels. Renewable hydrogen energy (H2) is becoming one of the better alternatives. Combustion of H2 for energy does not emit pollutant gases such as CO, , or . H2 has also been widely used in many sectors such as food, metallurgical, electronic, chemical, petroleum, and refinery industries. H2 has been technically demonstrated for transportation, heating, and power generation .
H2 yielded from the photocatalytic splitting of water has extensively received attention recently [2–4]. Since the H2 generation by the water electrochemical method was demonstrated, splitting of water photocatalyzed by TiO2 for the H2 fuel has been considered to be one of the alternates . The TiO2-based photocatalysts for H2 generation could be promoted by codoping of antimony and chromium , nickel and either tantalum or niobium , cobalt , Pt , and nitrogen . During photocatalysis, photo-excited holes can irreversibly oxidize electron donor compounds, and thus facilitate water reduction by conduction band electrons if the bottom of the conduction band of the photocatalyst is located at a more negative redox potential than the reduction potential of water . Inorganic reagents such as Na2S and Na2SO3 are generally used as the sacrificial compounds [12, 13].
In the present work, CuO and NiO were used as the promoters on the nanosize TiO2 to enhance catalytic splitting of water and seawater. Oxalic acid which may be formed from the photocatalytic reduction of CO2 in H2O was used as the sacrificial reagent during photocatalysis.
2. Materials and Methods
The CuO (2.5%) and NiO (2.5%) supported on nanosize TiO2 (P25) (UR, ITIT001) were prepared by the impregnation method. The samples were dried and calcined at 673 K for two hours to form CuO and NiO dispersed on TiO2 (CuO/nano-TiO2 and NiO/nano-TiO2), respectively. The X-ray diffraction (XRD) patterns of the photocatalysts were recorded on a XRD spectrometer using Cu Kα radiation () ranged from 10° to 80° (2θ) at the scanning speed of 5°/min.
The XANES spectra of the TiO2 photocatalysts were also recorded on the Wigler 17C beam line at the Taiwan National Synchrotron Radiation Research Center (NSRRC). The electron storage ring was operated at the energy of 1.5 GeV (ring current = 120–200 mA). A Si(111) double crystal monochromator was used for selection of energy at an energy resolution ( (eV/eV)) of . The absorption spectra were collected in ion chambers that were filled with helium and nitrogen mixed gases. Beam energy was calibrated by the adsorption edges of nickel and copper foils at the energy of 8335 and 8979 eV, respectively.
The photocatalytic splitting of water and seawater experiments was carried out in a quartz reactor (45 mL) having a total reflection mirror system. About 100 mg of the catalyst samples were dispersed in the simulated seawater (about 35 g of NaCl in the 1 L of pure water) under magnetic stirring for five hours. A 300 W Xenon arc lamp (Oriel Instruments, Model 6259) equipped with a water filter was used as the photocatalytic light source. The H2 gas generated from the photocatalytic splitting of water and seawater was analyzed by a gas chromatography (Varian 430-GC) equipped with a thermal conductivity detector. The apparent quantum efficiency (QE) of the photocatalysts was obtained by the equation QE (%) = (number of reacted electrons)/(number of incident photons) × 100 = (number of evolved H2 molecules × 2)/(number of incident photons) × 100.
3. Results and Discussion
The XRD patterns of the CuO/nano-TiO2 and NiO/nano-TiO2 photocatalysts are shown in Figure 1. The main diffraction peaks of the photocatalysts at (101), (200), (004), and (105) are observed, suggesting that the photocatalysts have mainly anatase crystallites. The XRD peaks of CuO and NiO are barely observed in the CuO/nano-TiO2 and NiO/nano-TiO2, which may be due to the existence of subnanosize CuO and NiO crystallites that are well dispersed on the nano-TiO2.
The XANES spectra of nickel and copper in the photocatalysts are shown in Figure 2. Metallic nickel (Ni) and copper (Cu) are not found. The absorption features observed at 8335 and 8979 eV suggest that NiO and CuO are the main nickel and copper species on the TiO2, respectively.
Figure 3 presents the photocatalytic splitting of water and seawater containing 0.05 M oxalic acid as the sacrificial reagent. On the nano-TiO2 photocatalyst, a very small amount of H2 is formed from the photocatalytic splitting of water and seawater. Notably, the accumulated H2 yielded from the photocatalytic splitting of water on CuO/nano-TiO2 and NiO/nano-TiO2 is about 32.4 and 3.07 μmol/gcat after the 5 h radiation, respectively. Compared to the photocatalytic splitting of seawater on CuO/nano-TiO2 and NiO/nano-TiO2, the accumulated H2 yields are less than those from water by 3.8 and 2.1 times, respectively. Hole scavenging with chlorides may occur during photocatalysis [14, 15]. Many hydroxyl groups such as TiOH2, TiOH on TiO2 may absorb Cl− to form TiCl, which may decrease the H2 yield in the photocatalysis [16, 17]. Generally, CuO on TiO2 can be reduced to Cu+ ( V) or Cu0 ( V) by attracting the excited electrons from the valence band of TiO2 during photooxidizing [18–21]. The reduction potential of NiO ( V) is slightly less than the TiO2 conduction band gap ( V) [22, 23]. Additionally, the reduction potential of H+/H2 ( V) is less than that of CuO or NiO. CuO and NiO can thus promote TiO2 in the photocatalytic H2 formation.
In the separate experiments, oxalic acid was formed from simultaneously photocatalytic reduction of H2O and CO2. It is of great interest to study the behavior of acetic acid as the sacrificial compound for photocatalytic splitting of water and seawater for the H2 fuel. Note that addition of sacrificial reagents in water or seawater may cause water pollution.
Effects of the oxalic acid sacrificial reagent concentrations on the photocatalytic splitting of water and seawater on CuO/nano-TiO2 are shown in Figure 4. Without oxalic acid, H2 may not be formed in the photocatalysis. A small amount of oxalic acid can enhance the H2 generation. Note that oxalic acid is a strong reductive reagent which may consume the photogenerated holes. After a 5 h UV-Vis irradiation, a better H2 yield from the photocatalytic splitting of water is about 42.4 μmol/gcat when the initial concentration of oxalic acid is 12.5 mM. However, the photocatalytic H2 formation from water and seawater affected by CuO and NiO promoted TiO2 was less than that of related studies, mainly due to the fact of the much less amount of the sacrificial reagents used in the photocatalysis. With an increase of the initial oxalic acid concentration by two times, the photocatalytic H2 generation is slightly decreased. As the initial concentration of oxalic acid is increased by four times, the H2 yields from the photocatalytic splitting of water are decreased by 24%. It seems that excessive oxalic acid sacrificial reagent may not have a positive effect on the photocatalytic splitting of water.
Photocatalytic splitting of seawater for H2 formation on CuO/nano-TiO2 and NiO/nano-TiO2 is feasible experimentally. The sacrificial reagent (oxalic acid) can enhance the H2 yields in the photocatalytic splitting of seawater. However, the excessive sacrificial reagent may not favor the photocatalysis. It is worth noting that a better H2 can be yielded from the photocatalytic splitting of seawater affected by CuO/nano-TiO2 (8.53 μmol/gcat) than that by NiO/nano-TiO2 (1.46 μmol/gcat). In particular, the hole scavenging with chlorides in seawater may be associated with the less H2 yielded from the seawater photocatalysis (on CuO/nano-TiO2) if compared with that from water (42.4 μmol/gcat).
The financial supports of the Taiwan National Science Council and Bureau of Energy are gratefully acknowledged.
- M. M. Hussain, I. Dincer, and X. Li, “A preliminary life cycle assessment of PEM fuel cell powered automobiles,” Applied Thermal Engineering, vol. 27, no. 13, pp. 2294–2299, 2007.
- S. J. Choung, J. Kim, and H. R. Kim, “The characterization and hydrogen production from water decomposition with methanol in a semi-batch type reactor using In, P-TiO2s,” International Journal of Photoenergy, vol. 2011, Article ID 359161, 7 pages, 2011.
- A. Y. Kim and M. Kang, “Effect of Al-Cu bimetallic components in a TiO2 framework for high hydrogen production on methanol/water photo-splitting,” International Journal of Photoenergy, vol. 2012, Article ID 618642, 9 pages, 2012.
- G. Lee, M. K. Yeo, M. H. Um, and M. Kang, “High-efficiently photoelectrochemical hydrogen production over Zn-incorporated TiO2 nanotubes,” International Journal of Photoenergy, vol. 2012, Article ID 843042, 10 pages, 2012.
- A. Fujishima and K. Honda, “Electrochemical photolysis of water at a semiconductor electrode,” Nature, vol. 238, no. 5358, pp. 37–38, 1972.
- H. Kato and A. Kudo, “Visible-light-response and photocatalytic activities of TiO2 and SrTiO3 photocatalysts codoped with antimony and chromium,” Journal of Physical Chemistry B, vol. 106, no. 19, pp. 5029–5034, 2002.
- R. Niishiro, H. Kato, and A. Kudo, “Nickel and either tantalum or niobium-codoped TiO2 and SrTiO3 photocatalysts with visible-light response for H2 or O2 evolution from aqueous solutions,” Physical Chemistry Chemical Physics, vol. 7, no. 10, pp. 2241–2245, 2005.
- Y. Wu, G. Lu, and S. Li, “The long-term photocatalytic stability of Co2+-modified P25-TiO2 powders for the H2 production from aqueous ethanol solution,” Journal of Photochemistry and Photobiology A, vol. 181, no. 2-3, pp. 263–267, 2006.
- M. Kitano, M. Takeuchi, M. Matsuoka, J. M. Thomas, and M. Anpo, “Photocatalytic water splitting using Pt-loaded visible light-responsive TiO2 thin film photocatalysts,” Catalysis Today, vol. 120, no. 2, pp. 133–138, 2007.
- T. Sreethawong, S. Laehsalee, and S. Chauadej, “Comparative investigation of mesoporous- and non-mesoporous-assembled TiO2 nanocrystals for photocatalytic H2 production over N-doped TiO2 under visible light irradiation,” International Journal of Hydrogen Energy, vol. 33, no. 21, pp. 5947–5957, 2008.
- K. Maeda and K. Domen, “New non-oxide photocatalysts designed for overall water splitting under visible light,” Journal of Physical Chemistry C, vol. 111, no. 22, pp. 7851–7861, 2007.
- S. Xu and D. D. Sun, “Significant improvement of photocatalytic hydrogen generation rate over TiO2 with deposited CuO,” International Journal of Hydrogen Energy, vol. 34, no. 15, pp. 6096–6104, 2009.
- H. Yan, J. Yang, G. Ma et al., “Visible-light-driven hydrogen production with extremely high quantum efficiency on Pt-PdS/CdS photocatalyst,” Journal of Catalysis, vol. 266, no. 2, pp. 165–168, 2009.
- A. Lair, C. Ferronato, J. M. Chovelon, and J. M. Herrmann, “Naphthalene degradation in water by heterogeneous photocatalysis: an investigation of the influence of inorganic anions,” Journal of Photochemistry and Photobiology A, vol. 193, no. 2-3, pp. 193–203, 2008.
- Y. Li, D. Gao, S. Peng, G. Lu, and S. Li, “Photocatalytic hydrogen evolution over Pt/Cd0.5Zn0.5S from saltwater using glucose as electron donor: an investigation of the influence of electrolyte NaCl,” International Journal of Hydrogen Energy, vol. 36, no. 7, pp. 4291–4297, 2011.
- M. R. Hoffmann, S. T. Martin, W. Choi, and D. W. Bahnemann, “Environmental applications of semiconductor photocatalysis,” Chemical Reviews, vol. 95, no. 1, pp. 69–96, 1995.
- Y. Li, F. He, S. Peng, D. Gao, G. Lu, and S. Li, “Effects of electrolyte NaCl on photocatalytic hydrogen evolution in the presence of electron donors over Pt/TiO2,” Journal of Molecular Catalysis A, vol. 341, no. 1-2, pp. 71–76, 2011.
- J. Yu, Y. Hai, and M. Jaroniec, “Photocatalytic hydrogen production over CuO-modified titania,” Journal of Colloid and Interface Science, vol. 357, no. 1, pp. 223–228, 2011.
- J. Yu and J. Ran, “Facile preparation and enhanced photocatalytic H2-production activity of Cu(OH)2 cluster modified TiO2,” Energy and Environmental Science, vol. 4, no. 4, pp. 1364–1371, 2011.
- H. J. Choi and M. Kang, “Hydrogen production from methanol/water decomposition in a liquid photosystem using the anatase structure of Cu loaded TiO2,” International Journal of Hydrogen Energy, vol. 32, no. 16, pp. 3841–3848, 2007.
- T. Sreethawong and S. Yoshikawa, “Comparative investigation on photocatalytic hydrogen evolution over Cu-, Pd-, and Au-loaded mesoporous TiO2 photocatalysts,” Catalysis Communications, vol. 6, no. 10, pp. 661–668, 2005.
- J. Yu, Y. Hai, and B. Cheng, “Enhanced photocatalytic H2-production activity of TiO2 by Ni(OH)2 cluster modification,” Journal of Physical Chemistry C, vol. 115, no. 11, pp. 4953–4958, 2011.
- W. Wang, S. Liu, L. Nie, B. Cheng, and J. Yu, “Enhanced photocatalytic H2-production activity of TiO2 using Ni(NO3)2 as an additive,” Physical Chemistry Chemical Physics, vol. 15, no. 29, pp. 12033–12039, 2013.