synthesis and structure of titania nanotubes for hydrogen generation
TRANSCRIPT
Synthesis and Structure of Titania Nanotubes for Hydrogen Generation
Sangworn Wantawee1,a,Pacharee Krongkitsiri2,b, Tippawan Saipin3,c, Buagun Samran1,d and Udom Tipparach1,*e
1Department of Physics, UbonRatchathani University, UbonRatchathani 34190 Thailand
2Department Department of Science and Mathematics, Faculty of Industry and Technology, Rajamangala University of Technology Isan, Phangkon, Sakonnakon, 47160, Thailand
3Department of Arts and Sciences, UbonRatchathani Technical College, Mueang District,UbonRatchathani Province 34000 Thailand
[email protected],[email protected], [email protected]@hotmail.com, e*[email protected]
Keywords:Titania nanotubes, TiO2, anodization, Hydrogen generation, Renewable energy
Abstract.Titania nanotubes (TiO2 NTs) working electrodes for hydrogen production by
photoelectrocatalytic water splitting were synthesized by means of anodization method. The
electrolytes were the mixtures of oxalic acid (H2C2O4), ammonium fluoride (NH4F), and sodium
sulphate(VI) (Na2SO4)with different pHs. A constant dc power supply at 20 V was used as anodic
voltage. The samples were annealed at 450 °C for 2 hrs. Scanning Electron Microscopy (SEM) and
X-ray diffraction (XRD) were used to characterized TiO2 NTs microstructure. TiO2 NTs with
diameter of 100 nm were obtained when pH 3 electrolyte consisting of 0.08 M oxalic acid, 0.5 wt%
NH4F, and 1.0 wt% Na2SO4 was used. Without external applied potential, the maximum photocurrent
density was 2.8 mA/cm2 under illumination of 100 mW/cm
2. Hydrogen was generated at an overall
photoconversion efficiency of 3.4 %.
Introduction
Conversion of sunlight to chemical energy in the form of hydrogen is a target of scientific and
technological interests which solutions may be feasible importance as a renewable source of
sustainable and environmentally energy for next generations. Photoelectrolysis of water to produce
hydrogen (H2) has attracted attention due to the depletion of fossil fuels and global warming. The
photocatalytic evolution of H2 and O2 from wateroccurs when a photocatalytic agent with appropriate
band gap is illuminated by sufficiently energetic light. Honda and Fujishima [1] demonstrated the
process of electrochemical photolysis of water using semiconductor TiO2 as a working anode.Since
then, a large number of semiconductor materials have been employed for photoanodes, also called
working anodes for hydrogen production. All of semiconductor materials, TiO2 and modified
structure TiO2 are widely used because they are highly photocatalytic, stable, abundant, and
environmentally safe [2].
The scientific principles for the hydrogen generation were established byBockris and Uosaki in
Bockris and Uosaki in 1976 [3], Bockris in 1980 [4], Bockris in 2003 [5], Bockris et al. in 1981 [6],
Gerischer in 1977 [7], and Chandra in 1985 [8] and reviewed by numerous literatures e.g., by
Linsebigler et al.in 1995 [9],Bak et al. in 2002 [10], and Nowotny et al. in 2007 [11]. Recently, most
of efforts have been focused on nanostructuredtitania such as nanoparticles [12], nanoflims [13], and
nanotubes [14-15] to increase water photo-splitting efficiency due to their high surface-to-volume
ratios and size-dependent properties in hoping to increase energy conversion efficiecy.
Nanostructured Titania may be synthesized by many methods [12-16] such as sol-gel, and
anodization. Anodization has been one of the most popular in making Titania nanotubes (TiO2 NTs).
We have recently prepared mesoporous of TiO2 electrodesby anodization [17]. It is believed that
ability to control the structures of TiO2 NTscan be expected to positively impact a variety of
importanttechnologies and the structures of TiO2 NTs depend largely on many preparation
Advanced Materials Research Vol. 741 (2013) pp 84-89Online available since 2013/Aug/30 at www.scientific.net© (2013) Trans Tech Publications, Switzerlanddoi:10.4028/www.scientific.net/AMR.741.84
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parameters such as temperature, electrolytes, and anodic voltages. In this paper, we present the effect
of electrolytes on the structures and photoelectrochemicalproperties of TiO2 NTs for hydrogen
production.
Experimental
TiO2 NTs were grown by anodization method at room temperature. Titanium sheet with 0.25 mm
thick, 99.7% purity purchased from Sigma Aldrich were firstly polished by various abrasive papers.
After polishing, polished Ti substrates were ultrasonically cleaned in the mixture of acetone and
ethanol. The mixed electrolytes consisting of 1/12 M C2O4H2�2H2O, 0.5wt% NH4F, and 1.0wt%
Na2SO4 with different pH values (3, 5, and 7) were used. The pH of the mixed electrolytes were
adjusted by addingappropriate amount of 1 M H2SO4, or 1 M NaOH.Titanium substrate samples were
anodized usinghome-made housing for the substrate. The system consists of a two-electrode
configuration with apiece of highly pure platinum counter electrode. The configuration of the set up
is shown in Fig. 1. This set up allows only one face of titaniun substrates contact with the electrolyte.
The anodization process was carried on under a constant dc potential 20 V for 2 hrs. Then, anodized
Ti substrates were rained by distilled water and dried in the flow of N2gas. All substrates were
annealed at 450 ˚C for 2 hrs to obtain anatase crystallinephases of TiO2 [13-16,]. The current and
anodization time data were collected computer-controlled apparatus equipped by LabVIEW
programming.To investigate the surface morphology and microstructure of TiO2NTs, all samples
were characterized by SEM and XRD techniques. The determine optical bandgap and
photocatalytic activity for water splitting of TiO2NTs the sample were characterized by UV-Vis and
I-V curve measurement.
Figure 1. Experimental equipment diagram of one-faceanodization for TiO2NTs
Advanced Materials Research Vol. 741 85
Results and Discussion
Fig. 1 shows XRD patterns of Ti sheet and post annealed TiO2 NTs. The XRD patterns show that the
phases of TiO2 NTs are anatase. The anatase (101) peak shows prominently when the anodization
Figure 2. XRD patterns of post annealed TiO2 NTs grown in the electrolytes with different pHs
Figure 3. SEM images of TiO2 NTs grown in the different pHelectrolytes (a) pH 5 and (b) pH 3.
0
500
1000
1500
2000
2500
20 30 40 50 60 70
Inte
nsi
ty (
A.U
.)
2Θ
Ti metal foil
TiO2 NTs pH 3
TiO2 NTs pH 7
TiO2 NTs pH 5A
(101)
A (
101)
A (
101
)
86 Materials and Nanotechnology in Engineering
Figure 4. Photocurrent densities of working electrodes made by TiO2 NTs grown in the different pH
electrolytes compared with the electrode made by Ti0.975 Fe0.025 O2sol-gel dip-coating film.
Figure 5. Photoconversion curves of working electrodes made by TiO2 NTs grown in the different
pH electrolytes compared with the electrode made by Ti0.975 Fe0.025 O2sol-gel dip-coating film.
was carried out in the electrolyte with pH 3. The SEM images of post-annealed TiO2 NTs grown in
the different pH electrolytes. The morphology of the TiO2 was found to be influenced by pH of the
anodizing electrolyte. The prepared samples with the anodization in pH 5 and pH 7 electrolytes were
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
-1.5 -1.0 -0.5 0.0 0.5 1.0 1.5
pH7
pH5pH3
Fe 2.5 %
Pho
tocu
rren
t d
ensi
ty (
mA
/cm
2)
Applied Potential (V)
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
-1.5 -1.0 -0.5 0.0 0.5 1.0 1.5
pH7
pH5pH3Fe 2.5 %
Photo
con
ver
sion E
ffic
ien
cy (
%)
Applied Potential (V)
Advanced Materials Research Vol. 741 87
the titania films with anatase phase. The TiO2 NTs were not observed while the samples with
anodization in pH 3 electrolyte showed clearly titania nanotubes (TiO2 NTs) with diameters of about
100 nm.
Photoconversionefficiency of TiO2 NTs was examined by a three-electrode cell at room
temperature under the illuminationof100 mW/cm2in a 1 M KOH solution. The photocurrent density
and applied potential (J-V) curves were shown in Fig. 4. The photoconversion efficiency of water
electrolysis was calculated based on the following relations [17-18],
η�%� = J� × �E� �� − �E�����
I�× 100%,
whereJph is the photocurrent density in mA/cm2,E� �� is the standard reversible potential which is 1.23
V, E��� is the applied potential obtained from equation, E��� =E� �� − E���, Emeasis the electrode
potential (vs. a reference electrode) of photoanode at which photocurrent is measured, Eaoc is the
electrode potential (vs. a reference electrode) of the same photoanode at open-circuit condition under
the same illumination and the sane electrolyte solution. I0 is the intensity of incident light of100
mW/cm2. The variation of the photoconversion efficiency curves as a function applied potential are
shown in Fig. 5. A maximum photoconversionefficiency of 3.4 % was obtained for TiO2 NTs
anodized in the electrolyte with pH 3. This photoconversion efficiency (3.4 %) of TiO2 NTs
photoanode is larger than that (0.8%) of nano-TiO2 film photoanode made by sol-gel dip coating [13,
19]. The increase of photoconversion efficiency may be resulted from the fact that the surface areas of
TiO2 NTs are larger than those ofnano-TiO2 films due to the agglomeration of the small spherical
crystals of nanoTiO2 crystals by nature [13]. Another reason may be due to the reduction of TiO2 NTs
optical bandgapenergy because nitrogen from NH4F used for making the electrolyte may incorporate
the structure of TiO2 NTs. It is well known that N-doped TiO2 lowers the bandgap energy of TiO2[20,
21] leading to increase the utilization of sunlight spectrums and also increase photoactivity. This may
be possible to identify the existence of nitrogen in the structure of TiO2 NTs by X-ray photoelectron
spectroscopy (XPS).
Summary
TiO2 NTs photoanodeshave been synthesized on titanium foils by anodization method in the mixtures
of oxalic acid (H2C2O4), ammonium fluoride (NH4F), and sodium sulphate(VI) (Na2SO4) with
different pHs. The post anodization process was carried out by anneaing in air at 450 °C for 2 hrs. The
best condition for growing TiO2 NTs was the electrolyte with pH 3. In this condition, the diameter of
prepared TiO2 NTs was about 100 nm. The phase of prepared TiO2 NTs was predominantly anatase.
The hydrogen production occurred with overall the photoconversion efficiency of 3.4 %.
Acknowledgements
The authors thank National Research Council of Thailand (NRCT) and Thailand Research Fund
(TRF)for funding. Sangworn Wantaweeand BuagunSamran would like to thank Faculty of Science
UbonRatchathani University for partially financial supports. One of the authors,
PachareeKrongkitsiri, would like to thank Department of Science and Mathematics, Faculty of
Industry and Technology, Rajamangala University of Technology Isan,Phangkon,
SakonnakonProvince for financial support and scholarship.
88 Materials and Nanotechnology in Engineering
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