Performance and Mechanism Research of Au-HSTiO2 on Photocatalytic Hydrogen Production

Ming-Xin LI Ren-Quan GUAN Jia-Xin LI Zhao ZHAO Jun-Kai ZHANG Cheng-Cheng DONG Yun-Feng QI Hong-Ju ZHAI

Citation:  Ming-Xin LI, Ren-Quan GUAN, Jia-Xin LI, Zhao ZHAO, Jun-Kai ZHANG, Cheng-Cheng DONG, Yun-Feng QI, Hong-Ju ZHAI. Performance and Mechanism Research of Au-HSTiO2 on Photocatalytic Hydrogen Production[J]. Chinese Journal of Structural Chemistry, 2020, 39(8): 1437-1443. doi: 10.14102/j.cnki.0254–5861.2011–2612 shu

Performance and Mechanism Research of Au-HSTiO2 on Photocatalytic Hydrogen Production

English

  • Economic development and industrialization led to a rapid improvement of living standards, but it also exposed energy crisis, which hindered sustainable development[1-3]. As an advanced environmental protection method, semiconductor photocatalysis technology has become a hot spot in hydrogen production[4-7]. Major breakthroughs in photocatalytic degradation have been achieved in catalytic desulphurization, photocatalytic water decomposition, photocatalytic reduction of organic compound synthesis, antibacterial effects, and so on.

    In related areas, photocatalytic semiconductors such as ZnO and TiO2 are widely used for many virtues[8-10]. First, TiO2 is safe, non-toxic and harmless to humans[10, 11]. Second, TiO2 is widely found in the earth's crust, cheap and low production costs. Unfortunately, the actual photocatalytic performance of TiO2 is much lower than urgent requirements[12-15]. For example, TiO2 can absorb most ultraviolet light, but only a small part of visible light can be absorbed, and photo-induced electrons can be easily recombined. Researchers propose many strategies to overcome these deficiencies. First, doping TiO2 with other substances (metal or non-metal elements and other semiconductors) can extend the lifetime of photogenerated electrons. Second, increasing the specific surface area of TiO2 makes more catalytic site proud exposure. The integration of above methods may be a desired strategy for improving photocatalytic performance.

    In general, the performance of a photocatalyst mainly depends on its chemical and physical structures, which is crucial for photon adsorption, charge carrier transfer, and catalytic surface reaction during photocatalysis. Until now, the deposition of precious metals such as Au, Pt, and Ag on the TiO2 surface can reduce the recombination rate of h+/e-, which extends the existence of electron holes and raises photocatalytic activity of TiO2[16-18]. Au is stable and not easy to accumulate in photocatalyst catalytic reactions. Under light irradiation, Au nanoparticles can extend the spectral response range of TiO2 from the ultraviolet region to the visible region, which further synergizes photocatalytic activity. The doping of high surface area TiO2 (HSTiO2) with Au is a preferable alternatives[19-22].

    In this study, Au-HSTiO2 was first used as a cocatalyst for photocatalytic hydrogen production. We prepared TiO2 with high specific surface area by sol-gel method, which has greater bandgap and photocatalytic activity based on quantum size effect. Au nanoparticles were deposited on HSTiO2 by liquid reduction method. Au-HSTiO2 was characterized by XRD, UV-vis, SEM, TEM, XPS and photocurrent intensity. The experimental results show that after 150 minutes radiation, Au-HSTiO2 has a photocatalytic hydrogen production with 5.129 mL H2.

    Methanol (99.9%), ethanol (99.9%), titanium dioxide (> 99.5%), sodium borohydride (99%), chloroauric acid (99%), tetrabutyl titanium (> 98%), hydrochloric acid (> 95%), acetic acid (> 95%) and polyethylene glycol(propanediol)-polyethylene glycol(propanediol)-polyethylene glycol(ethylene glycol)(F127) are supported by Shanghai Chemical Co., Ltd.. The dissolved water came from the analytical laboratory. All the above reagents are analytical levels.

    2.2.1   Synthesis of high specific surface area TiO2 (HSTiO2)

    The experimental method for obtaining HSTiO2 is as follows. First, 1.6 g of F127 was added to 30 mL ethanol, to which 3.5 mL of tetrabutyl titanium, 2.3 mL of acetic acid and 0.7 mL of hydrochloric acid were then further added. Second, the mixture was stirred at 60℃until completely dried. The beaker containing the mixed solution was placed in in an electric blast drying oven for 10 h and the sample was burned to 450 ℃ for 4 h at a heating rate of 5 ℃/min.

    2.2.2   Preparation of Au-HSTiO2

    In an ice water bath, 0.4 g HSTiO2 was dropped into a pale yellow HAuCl4 solution with a concentration of 3 mmol/L. Then 1 mL NaBH4 (0.1 mmol/L) was added to the above resulting solution followed by continuous stirring at a speed of 800 rpm. It can be observed that the solution gradually turns wine red under continuous stirring for 15 minutes, obtaining Au-HSTiO2 which was respectively washed with water and ethanol for 3 times each to remove ions. The Au-HSTiO2 was stirred at 60 ℃ until being completely dried.

    The pattern of the sample was obtained by X-ray diffraction pattern (XRD) through a Shimadzu XRD-6000 diffraction system having a high intensity CuKa radiation (40 kV, 200 mA) of 20~70 and a scanning step of 10 °/min. The surface morphology was discussed by scanning electron microscopy (SEM) (JSM-6510) at an accelerating voltage of 15 KV. The transmission electron microscopy (TEM) image was acquired on JEM-2100 transmission electron microscopy at an accelerating voltage of 200 kV. UV-vis diffuse reflectance spectra (DRS) were obtained on a Shimadzu UV-3600 spectrometer by using BaSO4 as a reference. X-ray photoelectron spectroscopy (XPS) was operated on PHI-5300 ESCA. Brunauer-Emmett-Teller (BET) surface area of the samples was determined from a N2 adsorption-desorption isotherm study at liquid nitrogen temperature (77 K) using Micromeritics TRiStarII3020.

    The H2 evolution experiments were carried out in the two-neck double walled borosilicate round-bottomed flask (100 mL) at room temperature. In order to prevent gas leakage from the reaction, the neck of the reactor was sealed with a rubber septum which is coated with vacuum silicone grease. A 300W Xe lamp was used as the artificial light source. 50 mg of photocatalyst was dispersed in aqueous methanol solution (CH3OH: H2O 1:3 by volume) by continuous stirring. Then He was bubbled through the reaction mixture for 30 minutes to fill the reactor with an inert gas. H2 evolution was sampled every 30 minutes for 150 minutes. The evolved hydrogen was detected by an on-line gas chromatograph (TECHCOMP GC7900) equipped with a thermal conductivity detector (TCD).

    Photoelectric electrochemical measurements were performed on the chi-760e electrochemical instrument of Shanghai Chenhua Instrument Co., Ltd.. Before the test was performed. The following steps were performed to prepare the electrode required for the test. 0.5 g sample was dispersed in 3 mL ethanol and evenly distributed on 1cm × 1cm fluorinated tin glass oxide electrode. After drying with a hairdryer, the resulting photocatalyst film was used as a working electrode, platinum as the counter electrode, and silver/silver chloride as the reference electrode. The 500W shaft lamp serves as a light source for lighting.

    Fig. 1 shows the XRD patterns to facilitate phase structures of prepared samples. Fig. 1a, 1b and 1c are diffraction patterns of TiO2, HSTiO2 and Au-HSTiO2, respectively. All the diffraction peaks of HSTiO2 (Fig. 1b) are consistent with TiO2 (Fig. 1a). All the diffraction peaks of Au-HSTiO2 (Fig. 1c) are well consistent with TiO2 and Au (JCPDS: 04-0784). It is fully proved that the Au-HSTiO2 sample is the composite structures of Au and TiO2 without other impurities.

    Figure 1

    Figure 1.  XRD patterns of (a) TiO2, (b) HSTiO2 and (c) Au-HSTiO2

    In order to study the morphology of Au-HSTiO2 composite photocatalyst, we presented its SEM and TEM images. As shown in Fig. 2a, Au nanoparticles adhere to the surface of flaky TiO2. We give TEM images (Fig. 2b) as further evidence. Au particles attach to TiO2 and bind closely to TiO2. It is well known that photocatalytic activity of photocatalysts is related to the lifetime of photo-producing electrons and holes. The structure of Au particles combined with TiO2 is conducive to extend the lifetime of photo-producing electrons, thereby increasing photocatalytic activity. The following work will confirm this inference.

    Figure 2

    Figure 2.  (a) SEM and (b) TEM images of Au-HSTiO2

    In order to explore the light absorption ability of different samples, ultraviolet absorption spectrum is given. As shown in Fig. 3, TiO2 and HSTiO2 samples show an intrinsic absorption peak in the UV region. The absorption peak of Au-HSTiO2 in the ultraviolet region is the same as that of TiO2. However, the Au-HSTiO2 sample exhibits absorption peaks from the ultraviolet region to the visible range. It can be concluded that Au-HSTiO2 has a wider light absorption area than TiO2 and can fully absorb visible light, resulting in higher photocatalytic activity.

    Figure 3

    Figure 3.  UV-visible absorption spectra of (a) TiO2, (b) HSTiO2 and (c) Au-HSTiO2

    The results of BET specific surface area data for TiO2, HSTiO2 and Au-HSTiO2 are shown in Fig. 4. The specific surface area values of TiO2, HSTiO2 and Au-HSTiO2 are 2.255, 121.122 and 88.124 m2·g−1, respectively. The results indicate HSTiO2 and Au-HSTiO2 prepared in our work possess high specific surface area.

    Figure 4

    Figure 4.  BET specific surface area data for TiO2, HSTiO2 and Au-HSTiO2

    To study the chemical composition of Au-HSTiO2, we used XPS to test the sample. The full spectrum of Au-HSTiO2 confirmed that the sample consisted of Au, O and Ti, and the XPS and XRD test results confirmed each other. The formation of Au-HSTiO2 heterostructure is demonstrated. In addition, the C element is derived from chamber contamination in the XPS device.

    Figure 5

    Figure 5.  XPS spectra of Au-HSTiO2

    Fig. 6 shows the yield of hydrogen produced by photocatalytic decomposition of water using TiO2, HSTiO2 and Au-HSTiO2, respectively with methanol as a hole scavenger. It can be concluded from the observation that after using a Xe lamp for 150 minutes, the amount of hydrogen generated by using Au-HSTiO2 as a photocatalyst to decompose water is much larger than that of TiO2 and HSTiO2. Compared with TiO2, the yield of hydrogen produced by Au-HSTiO2 as a photocatalyst decomposed water is increased by 24 times to 5.129 mL. The heterojunction structure of Au and HSTiO2 significantly increases the yield of hydrogen. In order to explore the cyclic stability of Au-HSTiO2, we conducted four cycles of experiments. After four cycles of test, the hydrogen generation capacity of the sample decreased slightly, which may be due to the shedding of gold nanoparticles. But overall, the sample has good cycle stability.

    Figure 6

    Figure 6.  (a) Time profile of photocatalytic H2 production through aqueous solution of methanol using Au-HSTiO2, (b) Cycle curve of the photocatalytic H2 production by Au-HSTiO2

    Fig. 7 shows photocurrent tests of TiO2, HSTiO2 and Au-HSTiO2. By comparing the photocurrent time curves of different samples in dark and visible light under the switching cycle mode, it can be concluded that Au-HSTiO2 has the highest photocurrent strength compared to TiO2 and HSTiO2. The results demonstrate that Au-HSTiO2 has higher electron hole separation efficiency, which leads to higher catalytic activity of Au-HSTiO2.

    Figure 7

    Figure 7.  Photocurrent response curves of (a) TiO2, (b) HSTiO2 and (c) Au-HSTiO2

    Fig. 8 shows the mechanism of Au-HSTiO2 composite photocatalytic hydrogen production. Under light conditions, the valence band (VB) electrons (e-) of titanium dioxide are excited to the conduction band (CB) and a hole (h+) is generated on the valence band. Because the gold has good electrical conductivity, the electrons on the titanium dioxide conduction band quickly transfer to Au, which has a good electron storage energy and effectively extends the lifetime of light producing electrons. The methanol group as a victim combines to the holes in the valence band to produce oxidation of methanol, which prevents the recombine of hole and electrons. The electrons generated by light react with the H+ adsorbed on the surface of the Au to form H2.

    Figure 8

    Figure 8.  Photocatalytic mechanism of the Au-HSTiO2 under visible light irradiation

    The Au-HSTiO2 composite photocatalyst was prepared successfully by liquid reduction method, and the photocatalytic properties of the material were good. The photocatalytic activity of Au-HSTiO2 was found to be the highest among composite materials. In short, Au-HSTiO2 is an excellent photocatalytic hydrogen production. This study also laid the foundation for further exploration of photocatalysts in the future.


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  • Figure 1  XRD patterns of (a) TiO2, (b) HSTiO2 and (c) Au-HSTiO2

    Figure 2  (a) SEM and (b) TEM images of Au-HSTiO2

    Figure 3  UV-visible absorption spectra of (a) TiO2, (b) HSTiO2 and (c) Au-HSTiO2

    Figure 4  BET specific surface area data for TiO2, HSTiO2 and Au-HSTiO2

    Figure 5  XPS spectra of Au-HSTiO2

    Figure 6  (a) Time profile of photocatalytic H2 production through aqueous solution of methanol using Au-HSTiO2, (b) Cycle curve of the photocatalytic H2 production by Au-HSTiO2

    Figure 7  Photocurrent response curves of (a) TiO2, (b) HSTiO2 and (c) Au-HSTiO2

    Figure 8  Photocatalytic mechanism of the Au-HSTiO2 under visible light irradiation

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  • 发布日期:  2020-08-01
  • 收稿日期:  2019-09-20
  • 接受日期:  2019-12-24
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