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nitric, sulphuric and phosphoric acids [18]. However, waste acids
from pre-treatment are harmful and corrosive pollutants for the
environment.
Recently, many researchers have reported that maximizing light
harness by the modification of TiO2 and improving acidity of the
semiconductor are feasible and cost-effective ways to improve
the photocatalytic activity of TiO2 [18–22]. Recently, Mao et al.
impurities and hydrogenation treatment [19]. Wang et al. have
reported that hydrogenated TiO2 nanoparticles introduce a sur-
face disorder structure, extending the light absorption to the near
infrared range (∼1200 nm) [22]. This modification process is clean,
however, the production of black TiO2 requires the hydrogenation
under the high pressure with the relatively high operation risk.
In this work, effective TiO2 nanoparticles with a dominant
anatase phase and a very small fraction of rutile phase has been
prepared by a sol-gel method and tested for the photocatalytic
degradation of phenol with the addition of hydrogen peroxide
(H2O2). The kinetics of heterogeneous photocatalytic processes
was studied by investigating the effect of operating parameters.
Moreover, the blue TiO2 nanoparticles have been developed under
atmosphere pressure with improved charge separation and the
photocatalytic activity. The efficiency of phenol degradation on
this blue TiO2 was higher than that of acidic pre-treated TiO2 with
sulphuric acid (H2SO4) and hydrochloric acid (HCl).
Fig. 1. The XRD patterns of the as-prepared TiO2 and the further hydrogenated blue
TiO2 samples.
the illuminated TiO2 nanoparticles was mixed with 150 ml of phe-
nol solution with initial concentration of 55 ppm (0.58 mM). Prior
to irradiation this solution was magnetically stirred in the dark for
about 30 min to reach the adsorption equilibrium so that the loss of
compound due to adsorption can be taken into account. A proper
volume of H2O2 was added to the solution at the initiation of irradi-
ation and compressed air was purged into the solution to maintain
aerobic condition. The light was provided by a 230-W high pressure
mercury UV lamp which its strongest emission light is with wave-
length of 254 nm. The distance from the UV lamp to the solution
was 8 cm. All experiments were conducted at room temperature
and about 3 ml of the aqueous solution was collected at regular
intervals and analyzed by UV–vis spectroscopy at wavelength of
269.5 nm. The samples were filtered through a Millipore membrane
filter with pore size of 0.1 m before the analysis.
2. Experimental
2.1. Catalyst preparation and characterization
The TiO2 nanoparticles were prepared by a sol-gel method.
Titanium (IV) isopropoxide (TTIP, >97%, Sigma–Aldrich) was firstly
dissolved in ethanol solvent (> 99.5%, Sigma–Aldrich) and distilled
water was added to the solution with a molar ratio of TTIP: ethanol:
water = 1:10:2. Hydrochloric acid (12.5 mol% in water, molar ratio
HCl:TTIP = 1:1) was added dropwise to adjust the pH under contin-
uous stirring for the hydrolysis process of the mixture in 30 min to
form sols. After aging for 24 h, the obtained gels were dried under
373 K overnight and then calcined at 773 K for 2 h to obtain TiO2
nanoparticles.
The Langmuir-Hinshelwood model is usually used to describe
the kinetics of photocatalytic reactions of aquatic organics
[7,23,24]:
The blue TiO2 nanoparticles were obtained after the hydrogena-
tion of TiO2 in H2 flow (80 mL/min) at 673 K for 24 h. The acidic
pre-treated TiO2 nanoparticles were produced by adding the par-
ent TiO2 into an acid solution (0.05 g TiO2 per mL 0.5 M H2SO4 or
1.0 M HCl) under sonication for 30 min and then dried overnight at
423 K for H2SO4 and 323 K for HCl.
The crystalline phases present in the TiO2 nanoparticles were
analyzed by a Shimadzu X-Ray Diffractometer (XRD-6000) with
CuK␣ radiation operated at 40 kV and 30 mA at scan range from 10
to 70 deg with continuous scanning mode at a rate of 2◦ min−1. The
surface area of the catalysts was measured by an Autosorb IQ-C sys-
tem according to the N2 adsorption isotherm at 77 K. An amount of
50 mg of the samples was degassed at 423 K for 12 h under vacuum
before the measurement. The morphology and size of solid catalysts
of the samples were observed with scanning electron microscopy
(SEM) which recorded on a FESEM, Zeiss Ultra+ and transmission
electron microscopy (TEM) by a Philips CM120 BioFilter. The crys-
tallographic structure of samples was imaged by a high resolution
transmission electron microscopy (HRTEM) by JEOL 2200FS.
dC
dt
krKadC
r = −
=
(1)
1 + Kad
C
where kr is the intrinsic rate constant, Kad is the adsorption equi-
librium constant and C is the concentration of aquatic organic.
When the initial concentration of phenol is low, Eq. (1) can be
simplified to the first-order kinetics with an apparent rate constant
kapp [7]:
ꢀ
ꢁ
C
ln
= −krKadt = −kapp
t
(2)
C0
The half-life time (degradation of phenol to its 50%) is calculated
by the following equation:
ln 2
t1/2
=
(3)
kapp
3. Results and discussion
3.1. TiO2 nanoparticles characterization
2.2. Photocatalytic activity test
The crystalline phases and crystallite size of both TiO2 and blue
TiO2 sample were determined from the X-ray diffraction patterns
(Fig. 1). The width of the peak obtained for both photocatalysts
was narrow which implies that crystalline structure is presented
Photodegradation of phenol was carried out in a 1.0 L capacity
cylindrical Pyrex-glass batch photoreactor. The proper amount of
Please cite this article in press as: H. Ling, et al., Photocatalytic degradation of phenol in water on as-prepared and surface modified