# Photocatalytic Properties of Size-Controlled Titania Nanotube Arrays

Authors: Takeshi Hashishin; Keisuke Misawa; Kazuo Kojima; Chihiro Yogi; Jun Tamaki
Journal: International Journal of Electrochemistry
 (2011)

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## Abstract

The titania nanotube arrays (TNAs) with smooth surface was synthesized by anodization of titanium foil with 3 cm2 in square area using the electrolyte composed of 0.2 wt% NH4F and 0.5 vol% H2SO4 in ethylene glycol in order to evaluate the methylene blue photodegradation under ultra-violet irradiation. The tube length and inner diameter as a size parameter were controlled by the anodization time from 5 to 10 h and applied voltage from 10 to 50 V. The titania nanotube arrays (TNAs) annealed at 300 to 500°C were assigned to anatase phase, and TNAs at 600°C had both phase of anatase and rutile. The crystallite size and the apparent rate constant were increased with the increase in the annealing temperature of TNAs from 300 to 500°C. The bigger crystallite size of TNAs is suggested to be related to the increase in the amount of hole at the valence band, leading to the decrease in the apparent rate constant of MB degradation. Interestingly, the four kinds of linear relationship with the apparent rate constant were seen in both the inner diameter of TNAs and the length. Consequently, the apparent rate constant strongly depended on inner diameter of TNAs.


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## Body

## 1. Introduction

Titanium oxide nanotube arrays prepared in an aqueous solution containing 0.5 to 3.5 wt% hydrofluoric acid by anodic oxidation were first reported by Gong et al. [1] The nanotube arrays with opened tops and closed bottom are desirable for applications due to their large surface areas and high reactivities. Recently, Roy et al. [2] and Rani et al. [3] reported the key functional features of titania nanotubes such as their growth, modification, and properties in the hundred articles related to electrochemically self-assembled titania nanotube arrays. The potential of their applications has therefore been evident for the wide fields: gas sensors [4–7], water photoelectrolysis [8–14], dye-sensitized and solid-state heterojunction solar cells [15–21], and biomedical materials [22].Anodized titania nanotube arrays have been synthesized in many different electrolytes: aqueous and organic solutions, and acidic and neutral ones, all of which contains fluoride ions [1, 23–26].  In a HF-based aqueous electrolyte, which has been the most frequently reported, nanotube growth has been limited up to a length of only 500 nm due to the strong chemical dissolution property of the titania layer into the solution; the titania film anodized at more than 30 V had no tube arrays structure [27, 28]. Recently, some neutral electrolytes have been used to fabricate longer titania nanotube arrays [26, 29, 30]. The neutral solutions, as a mild anodic oxidizing reactant, essentially suppress the chemical dissolution of the oxidized titania compared with acidic aqueous solutions [30]. Paulose et al. reported that a nanotube length of about 200 μm was obtained at 60 V by using an electrolyte composed of NH4F, water, and ethylene glycol; however, a 200 μm thick nanotube array film tended to peel off from the titanium substrate after drying in air due to the surface tension of water acting on the interface between the film and the substrate [26]. Thus, long nanotube arrays are unstable when dried in air. For many engineering applications, titania nanotube arrays require physical stability against drying or annealing; therefore, controlling the nanotube length is important. A free-standing titania nanotube layers with both ends open and a smooth surface were developed by applied voltage transition from 60 to 120 V [31]; however, there was no information on film thickness of the nanotube layer.There are only limited publications on the effect of the morphology of titania nanotube arrays on photocatalytic behavior [32, 33].  These reports showed the advantage over sol-gel films and the effects of crystallinity, tube length, and wall thickness on the degradation of dye aqueous solutions; however, the effect on the inner diameter was not specified.In the present work, we succeeded in preparation of the TNAs with no peeling off from the growth substrate of them, which were synthesized at 50 V for 5 h in an electrolyte composed of 0.2 wt% NH4F and 0.5 Vol% H2SO4 in ethylene glycol.  It was also possible to adjust the tube length and inner diameter by controlling the anodization time and applied voltage.  Furthermore, the effects of annealing temperature of TNAs and size parameters of the tube length, the inner diameter, and the wall thickness on the degradation of methylene blue in aqueous solution were also investigated in detail.


## 2. Experimental Procedure

The titania nanotube arrays (TNAs) were synthesized from titanium foil with 0.3 mm thick (99.5% purity; Nilaco).  Anodization was conducted at room temperature using the titanium foil as anode and an aluminum foil as cathode in an electrolyte solution of 0.2 wt% NH4F and 0.5 vol% H2SO4 in ethylene glycol.  A DC power of 10–50 V was supplied for 5–10 h to drive the anodization.  The TNAs synthesized were sonicated in ethanol, dried in air and then annealed at 300 to 600°C for 6 h.  The morphological features of the TNAs anodized were observed by means of FE-SEM (Hitachi S-4800), and their structural changes on annealing temperature were confirmed by means of X-ray diffraction (XRD, Rigaku RINT/DMAX-2200 X-ray diffractometer with Cu-Kμ radiation).  The photocatalytic properties of the TNAs obtained in different anodization and annealing conditions were evaluated from the photodegradation behavior of a methylene blue (MB) dye in aqueous solution.  These TNAs were immersed in an MB solution (1.63 × 10−5M, 3.5 mL) which had been placed in a quartz cell (10 × 10 × 65 mm3), and then, irradiated by a UV lamp (365 nm, 60 μW cm−2) at 25°C.  The solution was purged with oxygen for 60 min prior to UV irradiation, and the purging continued during irradiation.  The degradation of MB dye was monitored by absorbance at around 600–650 nm on a UV-Vis spectrometer (Shimadzu, UV-1700).


## 3. Results and Discussion

Since Zhang et al. [34] predicted two theories of kinetics of growth of anodic oxide films: the high field model (HFM) and the point defect model (PDM), the actual model of TNAs has been developed to explain the formation mechanism of TNAs based on anionic species containing fluoride ion, proton, and their complex, as discussed in many papers of Grimes et al. and Schmuki et al. listed in Section 1.  In the present work, the NH4F-H2SO4-EG system was chosen as an electrolyte suitable for the tube structure with smooth surface, in order to examine the results for the photocatalytic degradation of methylene blue using TNAs.Figure1 shows the typical surface morphologies and cross-sections of TNAs formed by anodization for 5 h using an electrolyte with/without 0.5 vol% sulfuric acid.  The array was vertically aligned to the titanium foil and was covered with entangled oxide layers fabricated by anodization in an electrolyte without H2SO4 as seen in Figure 1(a).  On the other hand, the addition of 0.5 vol% H2SO4 to the ethylene glycol solution was responsible for the surface smoothness of the nanotube array as shown in Figure 1(b).  As observed from these figures, the surface morphology was affected by the concentration of proton, as discussed by Cai et al. [28] and Yin et al. [35].FE-SEM images of titania nanotube arrays (TNAs) formed by anodization for 5 h in electrolyte solutions: (a) without H2SO4 at 20 V, (b) with H2SO4 at 20 V, and (c) with H2SO4 at 50 V. Insets show cross-sectional images.
(a)(b)(c)Figures1(b) and 1(c) show that increasing the applied voltage from 20 to 50 V increased the inner diameter of the resulting nanotube array from 37.3 to 110.3 nm by anodization for 5 h.  As shown in the insets, longer nanotube array can be formed at 50 V; the tube length also increased from 3.5 to 12.7 μm.  The size parameters of the TNAs anodized at 10–50 V for 5 h, tube length, inner diameter, wall-thickness, were measured using the scale bar of SEM images.  From the linear least squares fitting of these parameters, the correlation between the size parameters and applied voltage was calculated, showing the ratio of 321 nm/V in length, 2.33 nm/V in inner diameter, and 0.334 nm/V in wall-thickness. The growth rate for the TNAs anodized at 50 V for 5–10 h was 100 nm/h in length and 8.5 nm/h in inner diameter.Figure2 shows the X-ray diffraction (XRD) patterns and scanning electron microscopy (SEM) images of TNAs annealed at 300 to 600°C.  The TNAs annealed at 300 to 500°C were assigned to anatase phase of TiO2 (a=0.379 nm, c=0.951 nm; JSPDS 21-1272), and TNAs at 600°C had both phase of anatase and rutile (a=0.459 nm, c=0.296 nm; JCPDS 21-1276), as shown in Figure 2(a).  The respective tube wall-thickness of TNAs annealed at 300 and 400°C indicated 4.2 and 5.5 nm, which was calculated from the SEM images of Figures 2(b) and 2(c).  The tube wall-thickness at 500°C, 8.5 nm, from Figure 2(d), showed initiation of the particle formation of the tube wall.  On the other hand, the heat treatment at 600°C enlarged the tube wall-thickness from 8.5 to 13.2 nm.  As the result, the tube structure was collapsed completely.  The crystallite size (D) of TNAs annealed at 300 to 600°C was calculated from anatase 101 diffraction peak using Scherrer equation (D=Kλ/βcosθ; K=0.9), as shown in Figure 3(a).  The D value of TNAs annealed at 600°C, ca. 80 nm, was smaller than that of TNAs at 500°C, ca. 84 nm.  This behavior of crystallite size is similar to the temperature dependence of the anatase reported by Varghese et al. [36].  The lattice became 1.2-fold increasing in a-axis and 3.2-fold decreasing in c-axis by phase transition from anatase to rutile, leading to collapse the tubular structure.  The effects of annealing temperature of TNAs from 300 to 500°C on the photocatalytic degradation of methylene blue (MB) are shown in Figure 3(b).  From the linear least squares fitting of plots in Figure 3(b), it was obvious that the photodegradation of the MB obeys nearly the first-order reaction kinetics; ln(At/A0)=-kt.  From the slope of the linear fitting, the apparent rate constant of MB degradation was evaluated as 0.0014 min−1 (300°C), 0.0073 min−1 (400°C), and 0.011 min−1 (500°C).  These values were plotted in Figure 3(a) according to the right vertical axis.  The crystallite size and the apparent rate constant were increased with the increase in the annealing temperature of TNAs.  The size dependence of the fluorescence of the surface states in semiconductor nanoparticles indicated that the separation between electron-hole states (similar to the donor-acceptor pairs) increased upon decreasing particle size [37].  Consequently, the bigger crystallite size of TNAs is suggested to be related to the increase in the amount of hole at the valence band of TiO2, leading to the decrease in the apparent rate constant of MB degradation.  The plots of TNAs annealed at 500°C were slightly out of line, which depended on initiating the particle formation of the tube wall.  Therefore, the TNAs annealed at 400°C are adequate for evaluation of MB photodegradation.Figure 2
The titania nanotube arrays (TNAs) of as-anodized and annealed at 300 to 600°C: (a) X-ray diffraction patterns; (b,c,d,e) surface morphologies.Effects of annealing temperature of the titania nanotube arrays (TNAs) anodized at 20 V for 5 h (a) on the crystallite size of (101) diffraction peak and the rate constant, that is, the slope of (b), and (b) on the change of MB concentration as aln(At/A0) (at 365 nm) with ultra-violet irradiation time.
(a)(b)Figure4(a) shows the correlation between UV irradiation time and the MB photodegradation of the titania nanotube arrays (TNAs) annealed at 400°C for 6 h after anodized at 10–50 V for 5 h.  The respective plots of the TNAs anodized at 10–50 V for 5 h existed on the linear least squares fitting.  The apparent rate constant was calculated from the slope of five lines: 0.0050 min−1 (10 V), 0.0071 min−1 (20 V), 0.011 min−1 (30 V), 0.025 min−1 (40 V), and 0.026 min−1 (50 V).  The effects of the applied voltage of TNAs anodized for 5 h on the correlation between the inner diameter and the apparent rate constant are shown in Figure 4(b).  The apparent rate constant as a function of the length is also plotted in Figure 4(c).  Interestingly, the four kinds of linear relationship with the apparent rate constant were seen in both the inner diameter of TNAs and the length, which are categorized as regions A (0–10 V), B (10–30 V), C (30–40 V), and D (40–50 V).  The apparent rate constants at four regions were normalized as the unit of (min·mm·V)−1 including both factors of size and electric field, as summarized in Table 1.  The apparent rate constant strongly depended on inner diameter of TNAs.  Especially, the increase of the apparent rate constant was considerable in the slope change from region B to region C.  Generally, the EM wave absorber and dipole antenna for millimeter wave length are designed to correspond with the wave length of λ/4, denoting maximum absorbance in the phase difference of 90 degree.  The wave length of ultraviolet with maximum absorbance is 365 nm in this study.  The λ/4 of UV wave length (365 nm) is ca. 91 nm.  The drastic MB photodegradation appeared at the slope change from region B (66 nm in I. D.) to region C (85 nm in I. D.), suggesting that the wave length of λ/4 contributed to the efficient generation of hole on the surface of TNAs.Table 1
The dependence of rate constant on the inner diameter (I. D.) and the length of titania nanotube arrays.
RegionVoltage (V)k/I. D. (min·mm·V)−1k/Length (min·mm·V)−1A0–10280.71B10–306.10.050C30–40740.27D40–504.00.091Effects of the applied voltage of titania nanotube arrays (TNAs) anodized for 5 h (a) on the degree of MB degradation as aln(At/A0) (at 365 nm) with ultra-violet irradiation time, (b) on the correlation between the inner diameter and the apparent rate constant, that is, the slope of (a), and (c) on the apparent rate constant as a function of the length. The size and electric field factors of TNAs for the apparent rate constant of respective voltage regions are summarized in Table 1.
(a)(b)(c)In the previous study, we reported that the maximum absorption peak was blue shifted due to the formation of the demethylated compounds of MB in the photodegradation process of MB using titania thin film prepared by sol-gel method [38, 39].  In the present study, the similar blue shift was confirmed and therefore the demethylation of MB would occur.  Five different demethylated compounds such as Azure B, Azure A, N, N′-dimethylthionine (the isomer of Azure A), Azure C, and thionine could be formed by the demethylation reaction, but the correlation between these compounds and the morphology of titania nanotube array is still unclear.


## 4. Conclusion

We succeeded in the preparation of the titania nanotube arrays (TNAs) with no peeling off from the growth substrate of them, which in synthesized at 50 V for 5 h in an electrolyte composed of 0.2 wt% NH4F and 0.5 Vol% H2SO4 to ethylene glycol.  It was also possible to adjust the tube length and inner diameter by controlling the anodization time and applied voltage. The TNAs annealed at 300 to 500°C were assigned to anatase phase, and TNAs at 600°C had both phase of anatase and rutile.  The effects of annealing temperature of TNAs from 300 to 500°C on the photocatalytic degradation of methylene blue (MB) were investigated under UV irradiation with 365 nm.  The crystallite size and the apparent rate constant were increased with the increase in the annealing temperature of TNAs from 300 to 500°C.  The bigger crystallite size of TNAs is suggested to be related to the increase in the amount of hole at the valence band of TiO2, leading to the decrease in the apparent rate constant of MB degradation.  The effects of the applied voltage of TNAs anodized for 5 h on the correlation between the inner diameter and the apparent rate constant.  Interestingly, the four kinds of linear relationship with the apparent rate constant were seen in both the inner diameter of TNAs and the length. As a conclusion, the apparent rate constant strongly depended on inner diameter of TNAs.



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*Source: 656939-2011-08-10.xml*