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Journal of Energy Technologies and Policy
www.iiste.org
ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online)
Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013)

Hydrothermal Synthesis and Characterization of Onedimensional Ceria Nanorod for Chromium Ion Removal from
Wastewater
1,2*
1
1
2
Sujan Chowdhury

1.
2.

, Madiha Yasir , Mohammad Azmi B Bustam , Kuen-Song Lin

Department of Chemical Engineering, Universiti Teknologi PETRONAS, Bandar Seri Iskandar, 31750
Tronoh, Perak, Malaysia;
Department of Chemical Engineering & Materials Sciences, Yuan Ze University, Taiwan R.O.C.;
*Email address of corresponding author: sujan.chowdhury@petronas.com.my

Abstract
Remediation of wastewater contaminated with Cr(VI) species by ceria particles has received considerable
attention in recent years. The main objectives of the present study were to investigate the adsorption of Cr(VI)
species on the one-dimensional (1-D) ceria nanorod (CeNR). In where, CeNR has 20–40 nm in diameter and
200–300 nm in length, as confirmed through FE-SEM and TEM images. Higher surface area of CeNR is insisted
to the remediation of Cr(VI)-contaminated wastewaters. This work exemplifies the utilization of XAS and BET
to reveal the speciation of CeNR for further understands of the very complex adsorption process. It is also very
clear that decontamination of Cr species in wastewater via the in-situ remediation with CeNR permeable reactive
barriers would be environmentally attractive in the near future.
Keywords: Cr(VI)-contaminant, One-dimensional Ceria, Wastewater treatment; XANES/EXAFS.
1. Introduction
Growing pollution of the environment has led to intensive investigations into the immobilization or removal of
toxic substances from groundwater or waste streams. The interest seeking poisons in waste streams are heavymetal compounds, and some of them exhibit very hazardous properties. In soils and groundwater, chromium is
usually found and appears in the form of Cr(VI) and Cr(III), respectively from the effluent of industrial waste
water. In addition, chromium is toxic and considered as possible or probable carcinogens and/or mutagens (Di,
2006; Ponder, 2000; Wang, 2012). Conventional treatments of removing Cr species, such as chemical, biological
or membrane separation techniques are costly and non-effective. Reduction of chromium contaminated waste
water by oxidation nanoparticle has a great interest. Surface area of oxidation nanoparticle to the aqueous stream,
has been shown a promising electron-source material for the in-situ remediation of Cr(VI) contaminants in
groundwater. It follows that increasing the surface area of the nanophase ceria materials facilitate to increase the
remediation of chromium contaminated waste water for economical point of view. General physical and
chemical property of the oxidation nanomaterial such like ceria is specifically enhanced through the dimension
of the nanostructure with respect to their bulk like materials. The solvent composition and the cerium source are
of importance in the final product morphology (Chowdhury, 2011; Lin, 2010). The reaction temperature,
concentration of the cerium source, and reaction time has a significant influence on the yield of CeO2 nanorod
(Chowdhury, 2012; Zhang, 2006). The synthesis methods of CeO2 nanorods were relatively complicated and
always needed high-temperature, high-pressure or long-time treatments (Chowdhury, 2012; Chowdhury, 2011;
Lin, 2010; Qi, 2005). Therefore, the formation of 1-D ceria nanorods for chromium contaminated ground wastewater treatment application is still an ultimate challenge for cost-effective considerations. The X-ray absorption
spectroscopy (XAS) offers the basic knowledge of understanding the oxidation states and fine structures to a
study on the surface reaction of 1-D ceria nanorod. X-ray absorption spectroscopy is an excellent technique for
characterizing the valency and local structure of metals in 1-D ceria nanorod with a short-range order. X-ray
absorption near edge structure (XANES) spectroscopy provides information of electronic configuration,
stereochemistry and the oxidation states while, extended X-ray absorption fine structure (EXAFS) spectroscopy
can investigate the information on the atomic arrangement in terms of bond distance, number and kind of near
neighbors, thermal and static disorder.
Therefore, the main objective of the present study was to investigate the fine structures and oxidation states of 1D ceria nanorod particles for remediation of Cr contamination in simulated groundwater. The fine structures of
catalyst were also identified and characterized using X-ray diffraction (XRD), field-emission-scanning electron
microscopy (FE-SEM), Transmission electron microscopy (TEM), EXAFS or XANES techniques.
489
EESE-2013 is organised by International Society for Commerce, Industry & Engineering.
Journal of Energy Technologies and Policy
www.iiste.org
ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online)
Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013)

2. Method
2.1.

Materials and Preparation of Ceria Nanorod

In the typical procedure, Ce(NO3)3·6H2O solution (16 mmol, 10 mL) and higher concentration of NaOH solution
(14 M, 70 mL) were mixed in a 250 mL capacity Teflon-lined stainless steel autoclave, and left for one day at
100 oC in the digital temperature-controlled oven. The obtained one-dimensional nanorod product was washed
with DI water and dried at 60 oC for overnight and calcined at 300 oC for 3h in the presence of flowing air.
2.2.

Characterization and Analysis Techniques

Morphologies, crystallinities, particle size distribution, and the compositions of the commercial ceria powder and
as-synthesized 1-D CeNR catalysts were determined by FE–SEM equipped with EDS (Hitachi, S–4700 Type II)
and HR-TEM (Zeiss 10C). XRD patterns scanned from 5 to 90°(2θ) with a scan rate of 4°(2θ) min–1 with
monochromatic CuKα radiation (MAC Sience, MXP18) at 30 kV and 200 mA. The morphology and particle

size distribution of 1-D CeNR was determined by FE-SEM (Hitachi, S-4700 Type II) with a resolution of
0.1 nm. Nitrogen adsorption isotherms were measured at 77 K with ASAP2020 (Micromeritics Surface Area and
Porosity Analyzer). The pore size distribution was determined by the method of Barrett, Joyner, and Halenda
(BJH method). The XANES/EXAFS spectra were collected at the beamlines of 16A1 (Tender X-ray Absorption)

at the NSRRC of Taiwan. The electron storage ring was operated with energy of 1.5 GeV and a current of 100–
200 mA. The double crystal monochromator (DCM) was employed at beamline selected X-rays with energy
resolving power (E/∆E) higher than 7000 and sufficient for most XAS measurements. Data were collected in
fluorescence or transmission mode with a Lytle detector (Lytle, 1999) in the regions of the Ce(5723 eV) LIII-edge
at room temperature and analyzed with Athena. One-dimensional ceria nanorod was tested by adding the solid
directly to 100 mL of metal ion solution in a 125 mL HDPE bottle. Rate constants of kinetics study were
determined by adding 1 gm of CeNR to 500 mL K2Cr2O7 (Merck) solution at room temperature (ca. 25 °C).
Liquid samples were taken by a syringe every 5 min for about one hour and filtered through a 0.22 µm PVDF
syringe filter (Acrodisc). The concentrations of Cr ions of the samples were further characterized by ICP/AES
(Jobin Yvon Model JY32/38), AA (GBC Model 908).
3. Results and Discussion
Representative, TEM and FE-SEM micrographs of annealed ceria rod shape sample were obtained with widths
of 20–40 nm in diameter and 200–300 nm in length as shown in figure 1.

10

JCPDS-34-0394

20

30

40

50

60

70

80

[422]

[331]
[420]

[400]

[311]
[222]

[220]

(d)

[200]

(111)
(200)
(220)
(311)
(222)

Intensity (a.u.)

(c)

(b)

[111]

(a)

90

2Ɵ (degrees)
Figure 1. Microphotograph (a) TEM, (b) FE-SEM, (c) ED and (d) XRD of the ceria nanorod synthesized using
hydrothermal method at 100 oC for 24 h with further calcination at 300 oC for 3 h.
The continuous ring type electron diffraction (ED) pattern in figure 1(c) confirms the polycrystalline nature of
the CeNR and its face-centered cubic crystal structure. The XRD pattern of ceria nanorod is confirmed the
490
EESE-2013 is organised by International Society for Commerce, Industry & Engineering.
Journal of Energy Technologies and Policy
www.iiste.org
ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online)
Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013)

typical pattern of cubic fluorite-typed structure in figure 1(d). The average size of the crystalline ceria calculates
as based on the Scherrer formula was ~8 nm with the the feature peak appears at 28.55°, in correspondence with
the orientation (111) plane of CeNR structure. The BET specific surface area and pore volume of commercial
ceria nanomaterials and calcined CeNR were 6 and 78 m2g–1, respectively. CeNR provided a large surface area
and porous structures as compared with the different dimensional of ceria nanomaterials as shown in Table 1, so
that many active sites would be useful for the Cr(VI) contaminated waste water application.
Table 1: Cr(VI) adsorption capacities of ceria adsorbents
Maximum removal
Size (nm)
BET surface area
capacitiy (mg g-1)
(m2g-1)
Ceria microspheres
65.0
6.76
50-100
3D flowerlike
34.1
5.90
4000-6000
Ceria nanorod
74.0
11.60
100-200
* Pre-adjustment of the pH value is no long necessary (Xiao, 2009).
Adsorbent

pH
7
3
7

Normalized absorance (a.u.)

Generally, Ce LIII-edge EXAFS spectroscopy can provide the information on the atomic arrangement of sorbents
in terms of bond distance, coordination number, and kind of neighbors (Fernandez-García, 2002; Le Normand,
1988; Zhang, 2004). The XANES spectra for trivalent CeCl3, tetravalent commercial ceria and CeNR are
presented in figure 2. Trivalent CeCl3 is consisted with the strongest peak at about 5724.57 eV (figure 2(a)), due
to the dipole-allowed transition of Ce2p to Ce 4f15d final states and represented the 1-D CeNR (figure 2(c))
doesn’t match with the CeCl3 standard peak. In where, ceria nanostructure has consisted with mixed valence
state at the Ce-LIII edge in figure 2(b) and 2(c). The four observed peaks in the Ce LIII edge XANES have been
reported (Fernandez-García, 2002; Le Normand, 1988; Zhang, 2004). All samples have exhibited a double well
known white line characteristic of double cerium ground state as 4f0and 4f1 in agreement with the previous works
(Zhang, 2004). The LIII-edge positions of commercial ceria and CeNR are 5716.5, 5717.64, and 5719.07 eV,
respectively and are exhibited two clear peaks at 5727.5 ± 0.1 eV and 5737.4 ± 0.3 eV, respectively
(Fernandez-García, 2002; Le Normand, 1988; Shahin, 2004; Zhang, 2004). A significant change in the height of
the jump at the white line was observed in the 1-D CeNR samples. The change could be as a result of variation in
the morphology of the samples (Shahin, 2004). It is found that the LIII-edge points of all the samples are
consisted with the hybridization of 4f to 5d electronic state and as consisted with the electronic hole in 2p shell,
where, ṗ represents, as the electronic hole. The Ce 5d states are split in the cubic crystal field of the oxygen,
resulting in the low-energy shoulder. A peak in the pre-edge region at 5717.3 ± 0.2 eV with lower photon energy
can be obtained by curve fitting (Fernandez-García, 2002).

5727.7
5734.7

(c)

(b)

5724.9

(a)

5650

5700

5750

5800

5850

5900

Photon energy (eV)
Figure 2. XANES spectra of (a) CeCl3 standard, (b) commercial ceria powder, and (c) ceria nanorod synthesized
at 100 oC for 24 h with further calcination at 300 oC for 3 h.
The pre-edge region is assisted with the dipole-forbidden 2p3/2 → 4f transition, thus affects the 5d → 4f transition
state to form 4f15d1and 4f05d1electronic configuration (Shahin, 2004). In addition, peak position at 5723.64 ± 0.1
eV has been influenced with the 2p3/2 → 4f transition too and formed 2p4f15d0→2ṗ54f15d1transition (Bianconi,
1987). The variation of the particle morphology altered particle nucleation. Thus around ~2eV shift of binding
491
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Journal of Energy Technologies and Policy
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Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013)

energy has been occurred for CeNR from commercial ceria nanostructure. The intensities of the first peak of a
white line at 5727.5 ± 0.1 eV were due to the 2p4f15d0→2ṗ54f15d1transition, whereas the second peak at 5737.4
± 0.3 eV were due to a 2p4f05d0 →2ṗ64f05d1 transition (Shahin, 2004). In addition, fluorite structure of 1-D
CeNR Ce has 8 and 12 neighboring atoms in the first and second coordination shell corresponding to Ce-O and
Ce-Ce correlations (Fernandez-García, 2002).
It can be seen that Ce-O bond distance of 2.4 Å and the coordination number of 6.87 for the CeNR samples were
attenuated with the cerium and affordable existent with trivalent cerium oxide as shown in Table 2. Two
approaches were taken according to the fitting of the crystallographic data. In the first case, the coordination
number was held at the crystallographic values with the radial distance and Debye–Waller’s factors were varied.
Ceria nanoparticles have consisted with a bond length of 2.3 Å and a coordination number of 4.53. The apparent
shortening of the Ce-O bond length probably was caused by the random motion of the surface atom on Ce
particles instead of a true shortening of the bond distance. Moreover, bond distance of CeNR is approached to
trivalent cerium oxide and is larger than commercial ceria. That represent CeNR has higher content of trivalent
cerium oxide and that can effectively take to participate for Cr(VI) contaminated waste-water treatment.
Table 2. Structural parameters of ceria analyzed by EXAFS
CNa

CeCl3 standard
(Ce-O)
Commercial ceria (Ce-O)
1-D ceria- nanorod (Ce-O)

Rb(Å)

4.53
4.53
6.87

Bonding pair

2.32
2.32
2.41

2c

2

∆σ (Å )
0.00099
0.00086
0.00329

The effect of contact time on the amount of Cr(VI) adsorbed onto CeNR was measured at the different initial
concentration (20 to 80 ppm) in the presence of 1g of the one-dimensional ceria was added to 500 mL Cr(VI)
solution at room temperature as shown in figure 3. The adsorption rate was rather fast and Cr(VI) could be
removed after 160 min. This value is fairly higher than the bulk ceria to remove Cr(VI) due to the reflect of
higher surface area and oxidation state enhance the adsorption affinity of 1-D CeNR and the Cr(VI) species by
ion-exchange (Di, 2006; Jinhua, 2010; Xiao, 2009).
1.0

0.8

C/C0

(c)
0.6

(b)
(a)

0.4

0.2
0

40

80

120

160

Time (min)

Figure 3. Adsorption rate of Cr with different concentration (a) 20, (b) 40, and (c) 80 ppm respectively. CeNR
sample of 1g and 500 mL of aqueous solution have been taken at room temperature for adsorption analysis.
A simple kinetic analysis is performed with the aid of pseudo-second-order equation. In this equation, the value
of the rate constant k can be calculated in the form:

dq t
= k (q e − qt ) 2
dt
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Journal of Energy Technologies and Policy
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Where qe and qt are the amount of Cr(VI) adsorbed per unit mass (mg.g-1) of the adsorbent at equilibrium and
time t (min), respectively. After definite integration is applying the initial conditions qt = 0 at t = 0 and qt = qt at t
= t, Eq. (1) becomes

t
1
1
= 2 + t.
q t kq e q e

(2)

Nonlinear regressions using a least-squares fitting program (Origin 7.0, OriginLab Corp. Northampton, MA)
were conducted to acquire the best estimate of all constants for all the models. The fitting plots using pseudosecond-order equation is shown in figure 4. The kinetic parameters acquired from fitting results are summarized
12
in Table 3.
(A)

30

8

t/q (min g mg-1)

qe (mg g-1)

(B)

4

20

(b)
(c)
10

Non linear fitting
0
0
Experimental value
0

0

10

(a)

20

40

80

120

160

Time (min)
30

40

50

Ce (mg L-1)
Figure 4. (A) Adsorption isotherms of Cr(VI) and (B) pseudo-second order diffusion kinetic models for Cr with
different concentration of (a) 20, (b) 40, and (c) 80 ppm in the 1 g CeNR 500 mL solution at room temperature.
Concentration (ppm)

Table 3. Kinetic parameters of chromium contaminants
Rate constant, K (g.min-1 mg-1)
qe (mg.g-1)

Regression, R2

20

0.10

6.26

0.9991

40

0.03

10.75

0.9993

80
0.05
12.97
0.9997
-1
The maximum adsorption capacity (figure 4(a)) can be observed as 11.6 mg g and is consisted with higher
adsorption of Cr(VI) as compared with bulk ceria as shown in Table 1. In addition, Linear plots of the t/qt versus
t with linear regression coefficients is higher than 0.999 indicated the applicability of this kinetic equation and
the pseudo-second nature of the adsorption process for Cr(VI) onto CeNR and is closer to chemisorptions as
confirmed in the figure 4(b) and Table 3. This result suggested that higher BET surface area and oxygen vacancy
as revealed by XANES/EXAFS analysis from one-dimensional CeNR is facilitate the diffusion and adsorption of
Cr(VI) contaminated waste-water treatment (Xiao, 2009).
Conclusions
Morphology and structure of the ceria enhance the reactivity of the Cr(VI) from waste water enormously. The
FE-SEM photographs of 1-D CeNR catalysts used for the remediation of Cr-contaminated waste water indicated
ceria were nearly rod shape particles, which were 20–40 nm in diameter and 200–300 nm in length, respectively.
On the contrary, higher surface area is readily involved to the enhancement of Cr-contaminated wastewater
remediation. By XANES/EXAFS, it was found that mainly 1-D ceria possess higher oxidation states than
commercial ceria nanoparticle and thus may involve in the wastewater treatment. The high reaction rates and
493
EESE-2013 is organised by International Society for Commerce, Industry & Engineering.
Journal of Energy Technologies and Policy
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Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013)

significant removal of toxic Cr contaminants are suggested that the nanophase 1-D CeNR catalysts might be a
suitable material for in- situ remediation of Cr(VI) or Cr(III)-contaminated groundwater or waste streams.
Acknowledgements
Sujan Chowdhury and Madiha Yasir designed and conducted the experiments. Mohammad Azmi B Bustam and
Kuen-Song Lin revised the paper. All the authors discussed the results and commented on the menuscript. The
authors thanks to Yuan Ze University Taiwan R.O.C. and Universiti Teknologi PETRONAS, Malaysia to conduct
the research work.
References
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methanol interaction. Materials Chemistry and Physics 133(1), 163–169.
Chowdhury, S.,Lin, K. S. (2011). Synthesis and characterization of 1D ceria nanomaterials for CO oxidation and
steam reforming of methanol. Journal of Nanomaterials 2011.
Di, Z.-C., Ding, J., Peng, X.-J., Li, Y.-H., Luan, Z.-K.,Liang, J. (2006). Chromium adsorption by aligned carbon
nanotubes supported ceria nanoparticles. Chemosphere 62(5), 861–865.
Fernandez-García, M. (2002). XANES analysis of catalytic systems under reaction conditions. Catalysis
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Jinhua, W., Xiang, Z., Bing, Z., Yafei, Z., Rui, Z., Jindun, L.,Rongfeng, C. (2010). Rapid adsorption of Cr (VI)
on modified halloysite nanotubes. Desalination 259(1–3), 22–28.
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catalysts investigated by spectroscopic probes. The Journal of Physical Chemistry 92(9), 2561–2568.
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  • 1. Journal of Energy Technologies and Policy www.iiste.org ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online) Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013) Hydrothermal Synthesis and Characterization of Onedimensional Ceria Nanorod for Chromium Ion Removal from Wastewater 1,2* 1 1 2 Sujan Chowdhury 1. 2. , Madiha Yasir , Mohammad Azmi B Bustam , Kuen-Song Lin Department of Chemical Engineering, Universiti Teknologi PETRONAS, Bandar Seri Iskandar, 31750 Tronoh, Perak, Malaysia; Department of Chemical Engineering & Materials Sciences, Yuan Ze University, Taiwan R.O.C.; *Email address of corresponding author: sujan.chowdhury@petronas.com.my Abstract Remediation of wastewater contaminated with Cr(VI) species by ceria particles has received considerable attention in recent years. The main objectives of the present study were to investigate the adsorption of Cr(VI) species on the one-dimensional (1-D) ceria nanorod (CeNR). In where, CeNR has 20–40 nm in diameter and 200–300 nm in length, as confirmed through FE-SEM and TEM images. Higher surface area of CeNR is insisted to the remediation of Cr(VI)-contaminated wastewaters. This work exemplifies the utilization of XAS and BET to reveal the speciation of CeNR for further understands of the very complex adsorption process. It is also very clear that decontamination of Cr species in wastewater via the in-situ remediation with CeNR permeable reactive barriers would be environmentally attractive in the near future. Keywords: Cr(VI)-contaminant, One-dimensional Ceria, Wastewater treatment; XANES/EXAFS. 1. Introduction Growing pollution of the environment has led to intensive investigations into the immobilization or removal of toxic substances from groundwater or waste streams. The interest seeking poisons in waste streams are heavymetal compounds, and some of them exhibit very hazardous properties. In soils and groundwater, chromium is usually found and appears in the form of Cr(VI) and Cr(III), respectively from the effluent of industrial waste water. In addition, chromium is toxic and considered as possible or probable carcinogens and/or mutagens (Di, 2006; Ponder, 2000; Wang, 2012). Conventional treatments of removing Cr species, such as chemical, biological or membrane separation techniques are costly and non-effective. Reduction of chromium contaminated waste water by oxidation nanoparticle has a great interest. Surface area of oxidation nanoparticle to the aqueous stream, has been shown a promising electron-source material for the in-situ remediation of Cr(VI) contaminants in groundwater. It follows that increasing the surface area of the nanophase ceria materials facilitate to increase the remediation of chromium contaminated waste water for economical point of view. General physical and chemical property of the oxidation nanomaterial such like ceria is specifically enhanced through the dimension of the nanostructure with respect to their bulk like materials. The solvent composition and the cerium source are of importance in the final product morphology (Chowdhury, 2011; Lin, 2010). The reaction temperature, concentration of the cerium source, and reaction time has a significant influence on the yield of CeO2 nanorod (Chowdhury, 2012; Zhang, 2006). The synthesis methods of CeO2 nanorods were relatively complicated and always needed high-temperature, high-pressure or long-time treatments (Chowdhury, 2012; Chowdhury, 2011; Lin, 2010; Qi, 2005). Therefore, the formation of 1-D ceria nanorods for chromium contaminated ground wastewater treatment application is still an ultimate challenge for cost-effective considerations. The X-ray absorption spectroscopy (XAS) offers the basic knowledge of understanding the oxidation states and fine structures to a study on the surface reaction of 1-D ceria nanorod. X-ray absorption spectroscopy is an excellent technique for characterizing the valency and local structure of metals in 1-D ceria nanorod with a short-range order. X-ray absorption near edge structure (XANES) spectroscopy provides information of electronic configuration, stereochemistry and the oxidation states while, extended X-ray absorption fine structure (EXAFS) spectroscopy can investigate the information on the atomic arrangement in terms of bond distance, number and kind of near neighbors, thermal and static disorder. Therefore, the main objective of the present study was to investigate the fine structures and oxidation states of 1D ceria nanorod particles for remediation of Cr contamination in simulated groundwater. The fine structures of catalyst were also identified and characterized using X-ray diffraction (XRD), field-emission-scanning electron microscopy (FE-SEM), Transmission electron microscopy (TEM), EXAFS or XANES techniques. 489 EESE-2013 is organised by International Society for Commerce, Industry & Engineering.
  • 2. Journal of Energy Technologies and Policy www.iiste.org ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online) Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013) 2. Method 2.1. Materials and Preparation of Ceria Nanorod In the typical procedure, Ce(NO3)3·6H2O solution (16 mmol, 10 mL) and higher concentration of NaOH solution (14 M, 70 mL) were mixed in a 250 mL capacity Teflon-lined stainless steel autoclave, and left for one day at 100 oC in the digital temperature-controlled oven. The obtained one-dimensional nanorod product was washed with DI water and dried at 60 oC for overnight and calcined at 300 oC for 3h in the presence of flowing air. 2.2. Characterization and Analysis Techniques Morphologies, crystallinities, particle size distribution, and the compositions of the commercial ceria powder and as-synthesized 1-D CeNR catalysts were determined by FE–SEM equipped with EDS (Hitachi, S–4700 Type II) and HR-TEM (Zeiss 10C). XRD patterns scanned from 5 to 90°(2θ) with a scan rate of 4°(2θ) min–1 with monochromatic CuKα radiation (MAC Sience, MXP18) at 30 kV and 200 mA. The morphology and particle size distribution of 1-D CeNR was determined by FE-SEM (Hitachi, S-4700 Type II) with a resolution of 0.1 nm. Nitrogen adsorption isotherms were measured at 77 K with ASAP2020 (Micromeritics Surface Area and Porosity Analyzer). The pore size distribution was determined by the method of Barrett, Joyner, and Halenda (BJH method). The XANES/EXAFS spectra were collected at the beamlines of 16A1 (Tender X-ray Absorption) at the NSRRC of Taiwan. The electron storage ring was operated with energy of 1.5 GeV and a current of 100– 200 mA. The double crystal monochromator (DCM) was employed at beamline selected X-rays with energy resolving power (E/∆E) higher than 7000 and sufficient for most XAS measurements. Data were collected in fluorescence or transmission mode with a Lytle detector (Lytle, 1999) in the regions of the Ce(5723 eV) LIII-edge at room temperature and analyzed with Athena. One-dimensional ceria nanorod was tested by adding the solid directly to 100 mL of metal ion solution in a 125 mL HDPE bottle. Rate constants of kinetics study were determined by adding 1 gm of CeNR to 500 mL K2Cr2O7 (Merck) solution at room temperature (ca. 25 °C). Liquid samples were taken by a syringe every 5 min for about one hour and filtered through a 0.22 µm PVDF syringe filter (Acrodisc). The concentrations of Cr ions of the samples were further characterized by ICP/AES (Jobin Yvon Model JY32/38), AA (GBC Model 908). 3. Results and Discussion Representative, TEM and FE-SEM micrographs of annealed ceria rod shape sample were obtained with widths of 20–40 nm in diameter and 200–300 nm in length as shown in figure 1. 10 JCPDS-34-0394 20 30 40 50 60 70 80 [422] [331] [420] [400] [311] [222] [220] (d) [200] (111) (200) (220) (311) (222) Intensity (a.u.) (c) (b) [111] (a) 90 2Ɵ (degrees) Figure 1. Microphotograph (a) TEM, (b) FE-SEM, (c) ED and (d) XRD of the ceria nanorod synthesized using hydrothermal method at 100 oC for 24 h with further calcination at 300 oC for 3 h. The continuous ring type electron diffraction (ED) pattern in figure 1(c) confirms the polycrystalline nature of the CeNR and its face-centered cubic crystal structure. The XRD pattern of ceria nanorod is confirmed the 490 EESE-2013 is organised by International Society for Commerce, Industry & Engineering.
  • 3. Journal of Energy Technologies and Policy www.iiste.org ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online) Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013) typical pattern of cubic fluorite-typed structure in figure 1(d). The average size of the crystalline ceria calculates as based on the Scherrer formula was ~8 nm with the the feature peak appears at 28.55°, in correspondence with the orientation (111) plane of CeNR structure. The BET specific surface area and pore volume of commercial ceria nanomaterials and calcined CeNR were 6 and 78 m2g–1, respectively. CeNR provided a large surface area and porous structures as compared with the different dimensional of ceria nanomaterials as shown in Table 1, so that many active sites would be useful for the Cr(VI) contaminated waste water application. Table 1: Cr(VI) adsorption capacities of ceria adsorbents Maximum removal Size (nm) BET surface area capacitiy (mg g-1) (m2g-1) Ceria microspheres 65.0 6.76 50-100 3D flowerlike 34.1 5.90 4000-6000 Ceria nanorod 74.0 11.60 100-200 * Pre-adjustment of the pH value is no long necessary (Xiao, 2009). Adsorbent pH 7 3 7 Normalized absorance (a.u.) Generally, Ce LIII-edge EXAFS spectroscopy can provide the information on the atomic arrangement of sorbents in terms of bond distance, coordination number, and kind of neighbors (Fernandez-García, 2002; Le Normand, 1988; Zhang, 2004). The XANES spectra for trivalent CeCl3, tetravalent commercial ceria and CeNR are presented in figure 2. Trivalent CeCl3 is consisted with the strongest peak at about 5724.57 eV (figure 2(a)), due to the dipole-allowed transition of Ce2p to Ce 4f15d final states and represented the 1-D CeNR (figure 2(c)) doesn’t match with the CeCl3 standard peak. In where, ceria nanostructure has consisted with mixed valence state at the Ce-LIII edge in figure 2(b) and 2(c). The four observed peaks in the Ce LIII edge XANES have been reported (Fernandez-García, 2002; Le Normand, 1988; Zhang, 2004). All samples have exhibited a double well known white line characteristic of double cerium ground state as 4f0and 4f1 in agreement with the previous works (Zhang, 2004). The LIII-edge positions of commercial ceria and CeNR are 5716.5, 5717.64, and 5719.07 eV, respectively and are exhibited two clear peaks at 5727.5 ± 0.1 eV and 5737.4 ± 0.3 eV, respectively (Fernandez-García, 2002; Le Normand, 1988; Shahin, 2004; Zhang, 2004). A significant change in the height of the jump at the white line was observed in the 1-D CeNR samples. The change could be as a result of variation in the morphology of the samples (Shahin, 2004). It is found that the LIII-edge points of all the samples are consisted with the hybridization of 4f to 5d electronic state and as consisted with the electronic hole in 2p shell, where, ṗ represents, as the electronic hole. The Ce 5d states are split in the cubic crystal field of the oxygen, resulting in the low-energy shoulder. A peak in the pre-edge region at 5717.3 ± 0.2 eV with lower photon energy can be obtained by curve fitting (Fernandez-García, 2002). 5727.7 5734.7 (c) (b) 5724.9 (a) 5650 5700 5750 5800 5850 5900 Photon energy (eV) Figure 2. XANES spectra of (a) CeCl3 standard, (b) commercial ceria powder, and (c) ceria nanorod synthesized at 100 oC for 24 h with further calcination at 300 oC for 3 h. The pre-edge region is assisted with the dipole-forbidden 2p3/2 → 4f transition, thus affects the 5d → 4f transition state to form 4f15d1and 4f05d1electronic configuration (Shahin, 2004). In addition, peak position at 5723.64 ± 0.1 eV has been influenced with the 2p3/2 → 4f transition too and formed 2p4f15d0→2ṗ54f15d1transition (Bianconi, 1987). The variation of the particle morphology altered particle nucleation. Thus around ~2eV shift of binding 491 EESE-2013 is organised by International Society for Commerce, Industry & Engineering.
  • 4. Journal of Energy Technologies and Policy www.iiste.org ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online) Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013) energy has been occurred for CeNR from commercial ceria nanostructure. The intensities of the first peak of a white line at 5727.5 ± 0.1 eV were due to the 2p4f15d0→2ṗ54f15d1transition, whereas the second peak at 5737.4 ± 0.3 eV were due to a 2p4f05d0 →2ṗ64f05d1 transition (Shahin, 2004). In addition, fluorite structure of 1-D CeNR Ce has 8 and 12 neighboring atoms in the first and second coordination shell corresponding to Ce-O and Ce-Ce correlations (Fernandez-García, 2002). It can be seen that Ce-O bond distance of 2.4 Å and the coordination number of 6.87 for the CeNR samples were attenuated with the cerium and affordable existent with trivalent cerium oxide as shown in Table 2. Two approaches were taken according to the fitting of the crystallographic data. In the first case, the coordination number was held at the crystallographic values with the radial distance and Debye–Waller’s factors were varied. Ceria nanoparticles have consisted with a bond length of 2.3 Å and a coordination number of 4.53. The apparent shortening of the Ce-O bond length probably was caused by the random motion of the surface atom on Ce particles instead of a true shortening of the bond distance. Moreover, bond distance of CeNR is approached to trivalent cerium oxide and is larger than commercial ceria. That represent CeNR has higher content of trivalent cerium oxide and that can effectively take to participate for Cr(VI) contaminated waste-water treatment. Table 2. Structural parameters of ceria analyzed by EXAFS CNa CeCl3 standard (Ce-O) Commercial ceria (Ce-O) 1-D ceria- nanorod (Ce-O) Rb(Å) 4.53 4.53 6.87 Bonding pair 2.32 2.32 2.41 2c 2 ∆σ (Å ) 0.00099 0.00086 0.00329 The effect of contact time on the amount of Cr(VI) adsorbed onto CeNR was measured at the different initial concentration (20 to 80 ppm) in the presence of 1g of the one-dimensional ceria was added to 500 mL Cr(VI) solution at room temperature as shown in figure 3. The adsorption rate was rather fast and Cr(VI) could be removed after 160 min. This value is fairly higher than the bulk ceria to remove Cr(VI) due to the reflect of higher surface area and oxidation state enhance the adsorption affinity of 1-D CeNR and the Cr(VI) species by ion-exchange (Di, 2006; Jinhua, 2010; Xiao, 2009). 1.0 0.8 C/C0 (c) 0.6 (b) (a) 0.4 0.2 0 40 80 120 160 Time (min) Figure 3. Adsorption rate of Cr with different concentration (a) 20, (b) 40, and (c) 80 ppm respectively. CeNR sample of 1g and 500 mL of aqueous solution have been taken at room temperature for adsorption analysis. A simple kinetic analysis is performed with the aid of pseudo-second-order equation. In this equation, the value of the rate constant k can be calculated in the form: dq t = k (q e − qt ) 2 dt 492 EESE-2013 is organised by International Society for Commerce, Industry & Engineering. (1)
  • 5. Journal of Energy Technologies and Policy www.iiste.org ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online) Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013) Where qe and qt are the amount of Cr(VI) adsorbed per unit mass (mg.g-1) of the adsorbent at equilibrium and time t (min), respectively. After definite integration is applying the initial conditions qt = 0 at t = 0 and qt = qt at t = t, Eq. (1) becomes t 1 1 = 2 + t. q t kq e q e (2) Nonlinear regressions using a least-squares fitting program (Origin 7.0, OriginLab Corp. Northampton, MA) were conducted to acquire the best estimate of all constants for all the models. The fitting plots using pseudosecond-order equation is shown in figure 4. The kinetic parameters acquired from fitting results are summarized 12 in Table 3. (A) 30 8 t/q (min g mg-1) qe (mg g-1) (B) 4 20 (b) (c) 10 Non linear fitting 0 0 Experimental value 0 0 10 (a) 20 40 80 120 160 Time (min) 30 40 50 Ce (mg L-1) Figure 4. (A) Adsorption isotherms of Cr(VI) and (B) pseudo-second order diffusion kinetic models for Cr with different concentration of (a) 20, (b) 40, and (c) 80 ppm in the 1 g CeNR 500 mL solution at room temperature. Concentration (ppm) Table 3. Kinetic parameters of chromium contaminants Rate constant, K (g.min-1 mg-1) qe (mg.g-1) Regression, R2 20 0.10 6.26 0.9991 40 0.03 10.75 0.9993 80 0.05 12.97 0.9997 -1 The maximum adsorption capacity (figure 4(a)) can be observed as 11.6 mg g and is consisted with higher adsorption of Cr(VI) as compared with bulk ceria as shown in Table 1. In addition, Linear plots of the t/qt versus t with linear regression coefficients is higher than 0.999 indicated the applicability of this kinetic equation and the pseudo-second nature of the adsorption process for Cr(VI) onto CeNR and is closer to chemisorptions as confirmed in the figure 4(b) and Table 3. This result suggested that higher BET surface area and oxygen vacancy as revealed by XANES/EXAFS analysis from one-dimensional CeNR is facilitate the diffusion and adsorption of Cr(VI) contaminated waste-water treatment (Xiao, 2009). Conclusions Morphology and structure of the ceria enhance the reactivity of the Cr(VI) from waste water enormously. The FE-SEM photographs of 1-D CeNR catalysts used for the remediation of Cr-contaminated waste water indicated ceria were nearly rod shape particles, which were 20–40 nm in diameter and 200–300 nm in length, respectively. On the contrary, higher surface area is readily involved to the enhancement of Cr-contaminated wastewater remediation. By XANES/EXAFS, it was found that mainly 1-D ceria possess higher oxidation states than commercial ceria nanoparticle and thus may involve in the wastewater treatment. The high reaction rates and 493 EESE-2013 is organised by International Society for Commerce, Industry & Engineering.
  • 6. Journal of Energy Technologies and Policy www.iiste.org ISSN 2224-3232 (Paper) ISSN 2225-0573 (Online) Vol.3, No.11, 2013 – Special Issue for International Conference on Energy, Environment and Sustainable Economy (EESE 2013) significant removal of toxic Cr contaminants are suggested that the nanophase 1-D CeNR catalysts might be a suitable material for in- situ remediation of Cr(VI) or Cr(III)-contaminated groundwater or waste streams. Acknowledgements Sujan Chowdhury and Madiha Yasir designed and conducted the experiments. Mohammad Azmi B Bustam and Kuen-Song Lin revised the paper. All the authors discussed the results and commented on the menuscript. The authors thanks to Yuan Ze University Taiwan R.O.C. and Universiti Teknologi PETRONAS, Malaysia to conduct the research work. References Bianconi, A., Marcelli, A., Dexpert, H., Karnatak, R., Kotani, A., Jo, T.,Petiau, J. (1987). Specific intermediatevalence state of insulating 4f compounds detected by L3 x-ray absorption. Physical Review B 35(2), 806. Chowdhury, S.,Lin, K.-S. (2012). Characterization and surface reactivity analyses of ceria nanorod catalyst for methanol interaction. Materials Chemistry and Physics 133(1), 163–169. Chowdhury, S.,Lin, K. S. (2011). Synthesis and characterization of 1D ceria nanomaterials for CO oxidation and steam reforming of methanol. Journal of Nanomaterials 2011. Di, Z.-C., Ding, J., Peng, X.-J., Li, Y.-H., Luan, Z.-K.,Liang, J. (2006). Chromium adsorption by aligned carbon nanotubes supported ceria nanoparticles. Chemosphere 62(5), 861–865. Fernandez-García, M. (2002). XANES analysis of catalytic systems under reaction conditions. Catalysis Reviews-Science and Engineering 44(1), 59–121. Jinhua, W., Xiang, Z., Bing, Z., Yafei, Z., Rui, Z., Jindun, L.,Rongfeng, C. (2010). Rapid adsorption of Cr (VI) on modified halloysite nanotubes. Desalination 259(1–3), 22–28. Le Normand, F., Hilaire, L., Kili, K., Krill, G.,Maire, G. (1988). Oxidation state of cerium in cerium-based catalysts investigated by spectroscopic probes. The Journal of Physical Chemistry 92(9), 2561–2568. Lin, K. S.,Chowdhury, S. (2010). Synthesis, characterization, and application of 1-D cerium oxide nanomaterials: a review. International Journal of Molecular Science 11(9), 3226–32251. Lytle, F. W. (1999). The EXAFS family tree: A personal history of the development of extended X-ray absorption fine structure. Journal of Synchrotron Radiation 6(3), 123–134. Ponder, S. M., Darab, J. G.,Mallouk, T. E. (2000). Remediation of Cr(VI) and Pb(II) Aqueous Solutions Using Supported, Nanoscale Zero-valent Iron. Environmental Science & Technology 34(12), 2564–2569. Qi, R. J., Zhu, Y. J., Cheng, G. F.,Huang, Y. H. (2005). Sonochemical synthesis of single-crystalline CeOHCO3 rods and their thermal conversion to CeO2 rods. Nanotechnology 16(11), 2502–2506. Shahin, A. M., Grandjean, F., Long, G. J.,Schuman, T. P. (2004). Cerium LIII-Edge XAS Investigation of the Structure of Crystalline and Amorphous Cerium Oxides. Chemistry of Materials 17(2), 315–321. Wang, X., Wang, J., Chang, L., Ding, Q., Liu, H.,Jiang, X. (2012). Tunable synthesis of novel 3D CuI hierarchical architectures and their excellent Cr(VI) removal capabilities. RSC Advances 2(32), 12315– 12321. Xiao, H., Ai, Z.,Zhang, L. (2009). Nonaqueous sol−gel synthesized hierarchical CeO2 nanocrystal microspheres as novel adsorbents for wastewater treatment. Journal of Physical Chemistry C 113(38), 16625–16630. Zhang, D., Ni, X., Zheng, H., Zhang, X.,Song, J. (2006). Fabrication of rod-like CeO2: Characterization, optical and electrochemical properties. Solid State Sciences 8(11), 1290−1293. Zhang, F., Wang, P., Koberstein, J., Khalid, S.,Chan, S.-W. (2004). Cerium oxidation state in ceria nanoparticles studied with X-ray photoelectron spectroscopy and absorption near edge spectroscopy. Surface Science 563(1-3), 74–82. 494 EESE-2013 is organised by International Society for Commerce, Industry & Engineering.
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