3
60
H.R. Pouretedal et al. / Journal of Alloys and Compounds 513 (2012) 359–364
photocatalyst (SC) to the empty conduction band as the absorbed
photon energy, hꢀ, equals or exceeds the band-gap of the semi-
conductor photocatalyst leaving behind a hole in the valence band.
Thus in concert, electron and hole pair (e –h ) is generated. The
following chain reactions have been widely postulated [1,7,8].
The degradation efficiency of 2-nitrophenol determined with measurement of
absorbance of samples by a UV–vis spectrophotometer Carry-100 using a paired
1.0 cm quartz cell. The samples centrifuged to remove the nanoparticles before
absorbance measurement. The absorbance of samples before (Ao) and after a dis-
tinct time (At) of irradiation and Beers’ law to determination of Co and Ct use for
calculate of degradation efficiency (Eq. (7)).
−
+
Photoexcitation : MO /SC + hꢀ → e− + h+ M : Zr, Ce, Sn
ꢀ
ꢁ
ꢀ
ꢁ
(1)
(2)
(3)
(4)
2
Ct
At
%
Degradation = 100 × 1 −
= 100 × 1 −
(7)
Oxygen ionosorption : (O2)ads + e− → O2•−
Co
Ao
Ionization of water : H O → OH− + H+
The pH of samples, the dosage of catalysts and the presence of hydrogen per-
2
oxide investigated on the reactivity of photocatalysts. The hydrochloric acid and
sodium hydroxide (0.01 M) and a Metrohm pH-meter with combined electrode used
to control of samples pH at range of 3–9.
Protonation of superoxides : O2 + H+ → HOO•
•
−
The hydroperoxyl radical formed (Eq. (4)) also has scavenging
property as O2 thus doubly prolonging the lifetime of photohole:
3
. Results and discussion
HOO + e− → HO2−
HOO + H+ → H O
•
(5)
(6)
−
3.1. Characterization of nanoparticles
2
2
Both the oxidation and reduction can take place at the surface
of the photoexcited semiconductor photocatalyst. Recombination
between electron and hole occurs unless oxygen is available to
The X-ray diffraction patterns of SnO , ZrO and CeO2 nanopar-
ticles calcined at temperature of 550 C are indicated in Fig. 1A–C,
2
2
◦
respectively. As seen from Fig. 1A, the diffraction peaks of (1 1 0),
•
−
scavenge the electrons to form superoxides (O2 ), its protonated
◦
(
1 0 1), (2 1 1) and (1 1 2) at 2ꢂ of 26.8, 34.0, 51.8 and 64.8 , respec-
•
form the hydroperoxyl radical (HO2 ) and subsequently H O2
2
tively, show the formation of Cassiterite type tetragonal crystals
of SnO2 which matches well with JCPDS card # 41-1445 [18]. The
average of crystalline size (DT) is calculated 3.5 nm from the (1 1 0)T
diffraction peak using Scherrer’s equation (Eq. (8)) [19].
[
15,16].
In the light of the literature studies, this study was designed to
synthesis nanoparticles of ZrO , CeO2 and SnO2 by sol–gel proce-
2
dure. The different composition of prepared nanoparticles was used
in 2-nitrophenol photodegradation.
(
0.9ꢁ)
DT =
(8)
(
ˇ cos ꢂ)
2. Experimental
2
.1. Synthesis of nanoprticles
In Eq. (8), D is the average crystalline size in nm, ꢁ is the
radiation wavelength (0.154 nm), ˇ is the corrected half-width at
half-intensity and ꢂ is the diffraction peak angle.
The sol–gel method used to prepare of ZrO2, CeO2 and SnO2 nanoparticles. The
ammonium cerium (IV) nitrate ((NH4)2Ce(NO3)6, Merck), zirconium oxychloride
Zirconium dioxide is one of the most studied semiconductor
materials. Pure ZrO2 has a monoclinic crystal structure at room
temperature and transitions to tetragonal and cubic at increasing
temperatures [20]. The formation of crystalline forms of tetrag-
onal and monoclinic observes for ZrO2 nanoparticles calcined at
(
ZrOCl2·8H2O, Merck) and tin (IV) chloride (SnCl4·5H2O, Merck) used as starting
materials to prepare CeO2, ZrO2 and SnO2 nanoparticles, respectively. The 0.1 M
solutions of Ce(IV), Zr(IV) and Sn(IV) prepared and the nitric acid diluted solution
added drop by drop until these solutions became clear. Deionized and double dis-
tilled water used to prepare the solutions. The solutions aged overnight and are
called “sol”. Next, the ammonia solution (1:1) added drop by drop until the gel
samples obtained at pH of 7–8. The gel samples aged overnight. After aging, the
gel samples of Ce(OH)4, Zr(OH)4 and Sn(OH)4 dried at 100 C for 2 h and followed
by calcined at 550 C for 3 h. The light yellowish CeO2, white ZrO2 and white SnO2
nanoparticles obtained after calcinations process and then stored for further use.
◦
temperature 550 C (Fig. 1B). The tetragonal structure of ZrO2 can
◦
be considered as the distortion of the cubic structure of ZrO2 and
◦
◦
its adjacent diffraction-peak pairs ((0 0 2), (1 1 0)) at 34 , ((1 1 2),
(
◦
◦
2 0 0)) at 50 , and ((1 0 3), (2 1 1)) at 60 (2ꢂ), which originate
from the splitting of the cubic diffraction peaks of (2 0 0), (2 2 0)
and (3 1 1) [21,22]. The average crystallite size of ZrO2 crystal is
calculated from Debye–Scherrer formula [19] and found 12.3 nm.
2
.2. Characterization of nanoparticles
−
1
IR-spectra of ZrO2, CeO2 and SnO2 nanoparticles in range 4000–400 cm
recorded by using Nicolet Impact 400D FT-IR Spectrophotometer. A diffractome-
ter Bruker D8 ADVANCE Germany with anode of Cu (ꢁ = 1.5406 A˚ of Cu K␣) and
Fig. 1C show the XRD pattern of nanosized CeO powder in 2ꢂ
2
◦
◦
◦
◦
◦
◦
of 20–80 . The five peaks with 2ꢂ values of 28.6 , 33.2 , 47.5 , 56.4
and 59.2 correspond to the (1 1 1), (2 0 0), (2 2 0), (3 1 1) and (2 2 2)
filter of Ni applied to record of X-ray diffraction (XRD) patterns of nanoparticles.
A JEOL JEM-1200EXII transmission electron microscope (TEM) operating at 120 kV
use for estimation of nanoparticles size. The supporting grids were formvar-covered,
carbon-coated, 200-mesh copper grids. BET (Brunauer–Emmett–Teller) surface area
of nanoparticles determined by using Monosorb Quantochorom.
planes indicate the formation of pure-phase CeO in a cubic fluorite
2
structure [23,24]. It is clear that all Bragg reflections for sample
agree well with those of standard CeO2 and noticeably broadened
of all reflections show the fine nature of CeO2 particles. The size of
CeO2 particles is obtained 8.2 nm by Debye–Scherrer formula.
2
.3. Photocatalytic activity of nanoprticles
The photocatalytic activity of prepared nanoprticles studied in photodegra-
The transmission electron microscopy images of SnO , ZrO2
2
dation of 2-nitrophenol. Phenol and its derivatives such as 2-nitrophenol are
industrially important chemicals and thus their presence in the environment is rela-
tively very common. Due to their high toxicity, they represent a group of dangerous
chemicals even at low concentrations [17].
and CeO2 nanoparticles are shown in Fig. 2A–C, respectively. The
spherical topography saw from the TEM images for prepared
nanoparticles. The formation of nanoparticles with size less than
20 nm confirmed by TEM images that agreement with results of
XRD analysis. The TEM analysis also shows a slightly irregular
and rounded shape for synthesized nanoparticles. The IR spec-
Photodegradation experiments perform in a photocatalytic reactor system. A
0 W mercury low pressure lamp uses as irradiation source. The lamp and the tube
7
immersed in the photoreactor cell with a light path of 3.0 cm. The photoreactor
filled with 50 ml of 10–50 mg/L of 2-nitrophenol and 0.1–0.8 g/L of photocatalysts.
The ZrO2, CeO2, SnO2 and mixture of ZrO2/CeO2, ZrO2/SnO2 and CeO2/SnO2 use as
photocatalysts. The whole reactor cooled with a water-cooled jacket on its outside
tra of prepared nanoparticles of SnO , ZrO and CeO2 showed an
2
2
1
−
absorption band at range of 500–450 cm that is related to the
vibration of M–O–M bond in MO2 with M: Sn, Zr and Ce [25,26].
BET (Brunauer–Emmett–Teller) surface area of prepared photocat-
◦
and the temperature was kept at 25 C. All reactants in the reactions stir using a
magnetic stirrer for ensure that the suspension of the catalyst was uniform during
the course of the reaction. In order to setting the adsorption/desorption equilib-
rium of 2-nitrophenol on heterogeneous catalysts surface, the reactor keep in dark
conditions within 30 min.
alysts determined by using Monosorb Quantochorom and obtained
2
2
63.4, 254.6 and 231.8 m /g for SnO , ZrO and CeO , respectively.
2
2
2