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Accepted Manuscript
Title: Preparation and characterization of Pd doped ceria-ZnOnanocomposite catalyst for methyl tert-butyl ether (MTBE)photodegradation
Author: Zaki S. Seddigi Ali Bumajdad Shahid P. Ansari SalehA. Ahmed Ekram Danish Naeema H. Yarkandi ShakeelAhmed
PII: S0304-3894(13)00821-2DOI: http://dx.doi.org/doi:10.1016/j.jhazmat.2013.10.070Reference: HAZMAT 15520
To appear in: Journal of Hazardous Materials
Received date: 24-9-2013Revised date: 27-10-2013Accepted date: 29-10-2013
Please cite this article as: Z.S. Seddigi, A. Bumajdad, S.P. Ansari, S.A.Ahmed, E. Danish, N.H. Yarkandi, S. Ahmed, Preparation and characterizationof Pd doped ceria-ZnO nanocomposite catalyst for methyl tert-butylether (MTBE) photodegradation, Journal of Hazardous Materials (2013),http://dx.doi.org/10.1016/j.jhazmat.2013.10.070
This is a PDF file of an unedited manuscript that has been accepted for publication.As a service to our customers we are providing this early version of the manuscript.The manuscript will undergo copyediting, typesetting, and review of the resulting proofbefore it is published in its final form. Please note that during the production processerrors may be discovered which could affect the content, and all legal disclaimers thatapply to the journal pertain.
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Preparation and characterization of Pd doped ceria-ZnO nanocomposite catalyst
for methyl tert-butyl ether (MTBE) photodegradation
Zaki S. Seddigi1, Ali Bumajdad2, Shahid P. Ansari1, Saleh A. Ahmed1*, Ekram Danish3
Naeema H. Yarkandi1 and Shakeel Ahmed4
1Chemistry Department, Umm Al-Qura University, Makkah, Saudi Arabia.
2Chemistry Department, Faculty of Science, Kuwait University, Kuwait3Chemistry Department, King Abdulaziz University, Jeddah, Saudi Arabia4Center for Refining & Petrochemicals, Research Institute, King Fahd University of Petroleum & Minerals, Dhahran 31261, Saudi Arabia
*Corresponding Author’s e-mail: [email protected]
Abstract
A series of binary oxide catalysts (ceria-ZnO) were prepared and doped with different
amounts of palladium in the range of 0.5% to 1.5%. The prepared catalysts were
characterized by SEM, TEM, XRD and XPS, as well as a N2 sorptiometry study. The
XPS results confirmed the structure of the Pd CeO2-x-ZnO. The photocatalytic activity of
these catalysts was evaluated for degradation of MTBE in water. These photocatalyst
efficiently degrade a 100 ppm aqueous solution of MTBE upon UV irradiation for five
hours in the presence of 100 mg of each of these photocatalysts. The removal of 99.6% of
the MTBE was achieved with the ceria-ZnO catalyst doped with 1% Pd. In addition to the
Pd loading, the N2 sorptiometry study introduced other factors that might affect the
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catalytic efficiency is the catalyst average pore sizes. The photoreaction was determined
to be a first order reaction.
Keywords: Binary oxide catalyst; Zinc Oxide; Cerium oxide; Catalyst;
Photodegradation; MTBE.
1. Introduction
The steep increase in the concentration of pollutants in the environment has attracted
considerable interest from researchers seeking to discover efficient methods for
controlling the entry of pollutants and reducing the existing pollutant load in the
environment [1- 5]. Several decades ago, fuel oxygenates were introduced to eliminate
the use of leaded gasoline, and these molecules helped to improve the octane value of
gasoline and provide nearly complete combustion of fuel by supplying extra oxygen
during the combustion process [6]. After the passage of the clean air act in 1990, their use
increased tremendously [7]. In 1997, after the Kyoto protocol agreement to control the
emission of greenhouse gases, fuel oxygenates were in high demand worldwide [8].
There are two types of fuel oxygenates, including aliphatic alcohols and ethers. The
blending of alcohols in gasoline required careful handling to avoid water content.
However, ether is easy to mix with gasoline without any problems. Therefore, ether based
oxygenates, such as ethyl tert-butyl ether and methyl tert-butyl ether, were preferentially
blended with gasoline [9, 10]. As the application of MTBE became more common and its
consumption increased, MTBE began to appear in certain water sources, which raised
concern over human health and its increasing concentration in water bodies [11, 12].
Therefore, MTBE was being considered a potential environmental pollutant because it
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found its way into the environment via accidents, spills, faulty gas station and leakage
from pipelines. The main reason for its accumulation in water bodies was due to its high
solubility in water water ( 50 mgl-1) [13]. MTBE has very weak partition with the
organic fraction in soil, and once released from a source, it has a tendency to spread
rapidly in groundwater where its presence in water poses a high risk to human health.
MTBE has a high affinity for blood resulting in a tendency to accumulate in the blood
stream, which can be detected during breathing. Human exposure to MTBE may result in
coughing, dizziness, fever, headaches, muscular aches, vomiting, sleepiness and skin and
eye irritation [14, 15]. In the light of available reports, there are no data on human
carcinogenicity but the evidences of exposure of MTBE on mice and rats have
demonstrated the carcinogenicity and therefore, human carcinogenic nature of MTBE
cannot be ruled out. MTBE concentration for carcinogenicity varies depending on subject
and condition and it can be broadly grouped as concentration higher than 300 ppm but
below this concentration and above the advised concentration by EPA (20-40 ppb) it is
toxic to human on long term exposure. Therefore, The United States Environment
Protection Agency (USEPA) has also suggested that at higher concentrations, MTBE
may be carcinogenic [16, 17]. In addition, MTBE affects the taste and odor of water.
Based on taste and odor, the USEPA has issued limits for MTBE in drinking water in the
range of 20-40 ppb [18, 19]. The special characteristics of MTBE and its effects on the
environment and human health have attracted much interested from scientists seeking to
control its entry into the environment and to degrade the MTBE currently in the
environment. Previously, different conventional techniques have been used with limited
success including activated carbon treatments, aerobic/anaerobic biodegradation, air-
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stripping to remove MTBE from water [20, 21]. MTBE was determined to be highly
resistant to biodegradation due to its ether linkage and tertiary carbon. In addition, MTBE
has a high solubility in water, a very low Henry’s law constant (5.5 x 10-4 atm m3mol-1 at
25 °C), which hinders its partition from the liquid phase to the vapor phase, and a
moderate affinity toward carbon, which resulting in the high cost of activated carbon
adsorption [22, 24].
Recently, heterogeneous photocatalysis, which is an advanced oxidation processes
(AOP), has become widely applied to the treatment of toxic and non-biodegradable
compounds from the environment. Photocatalysis is a simple and very promising
technique for solving various environmental and energy issues. Environmental pollution
as well as the problems associated with the presence and ever increasing mass/volume of
organic, toxic and nonbiodegradable pollutants provide the impetus for fundamental and
applied research to solve these issues [25]. Typically, photocatalysis is initiated by the
irradiation of a photocatalyst, which are primarily composed of semiconducting metal
oxides, with a light source with sufficient energy to excite an electron from the valence
band of the photocatalyst to the conduction band, which creates a hole in the valence
band. Therefore, the electron-hole pair is generated due to photoexcitation and reacts with
hydroxyl ions/oxygen/water to produce hydroxyl (•OH) radicals. These hydroxyl (•OH)
radicals react with the organic molecules adsorbed on the photocatalyst and degrade them
to CO2 and H2O through a series of chemical reactions. Many metal oxides have been
reported to be active photocatalysts for the degradation of organic pollutants. However,
each of these photocatalysts has its own drawbacks that limit its usage under particular
conditions [26, 27]. In addition, a rare earth cerium oxide (CeO2) has also been studied
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and applied in heterogeneous catalysis due to its ability to release and absorb oxygen
through a fast Ce4+/ Ce3+ cycle [28- 30]. Recently, ceria-ZnO composites have been
reported to exhibit enhanced photoactivity in the photocatalytic degradation of
Rhodamine B by Li et al. [31] compared to their individual components, which might be
due to improved separation of the photogenerated electron/hole pairs, larger surface area
and enhanced adsorption ability of the surfaces and interfaces in nanosize ceria-ZnO.
Noble metal (Pt, Rh, Pd) doping on ceria, which can be used as a support or promoter, is
very important due to the unique acid-base and redox properties of ceria that further
influences the redox reactions of supported noble metals, the catalytic property of metal
crystallites, the thermal resistance of supporting material and dispersion of supported
metals [32]. In addition, Pd loading onto ceria has been reported to alter the surface
properties of the support material due to the electron-transfers between Ce and Pd [33].
Therefore, encouraged by the properties described above, we synthesized a novel catalyst
by combining CeO2 and ZnO and doped it with different amount of Pd to study the
photocatalytic degradation and kinetics of MTBE in the presence of UV radiation.
2. Experimental:
2.1. Materials
Cerium nitrate hexahydrate, zinc nitrate hexahydrate and methyl tert-butyl ether (MTBE)
were obtained from Sigma-Aldrich, USA in 99.9% purity. Palladium (II) nitrate dihydrate
was obtained from Merck and double distilled water were used in this work.
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2.2. Preparation of the Catalyst
Palladium doped composite ceria-ZnO photocatalyst nanoparticles were prepared via a
co-precipitation method. In a typical co-precipitation method, an aqueous solution of the
required molar ratios of zinc nitrate hexahydrate and cerium nitrate hexahydrate are
mixed with continuous stirring at room temperature for 2 hours. In addition, a small
amount of ethylene glycol was added as a structure modifying agent to the above
solution. Then, an appropriate amount of sodium carbonate was added to the solution to
obtain a pH of 10.0. A precipitate was formed and separated by centrifugation. The
prepared precipitates, which are the precursors of the ceria-ZnO composite, were
thoroughly washed with de-ionized water and then with ethanol. The prepared
precipitates were dried in air at 100 °C overnight. The dried ceria-ZnO composite
precursors were calcined at 450 °C for 6 hours to obtain the ceria-ZnO particles.
Palladium was impregnated onto the composite oxide using the incipient wetness
impregnation method. The Pd loadings ranged from 0.5% to 1.5% based on the weight of
the composite ceria-ZnO support.
2.3. Photocatalytic Reaction Procedure
Methyl tert-butyl ether used in the photodegradation experiments was used as received
from Aldrich. A 100 ppm MTBE stock solution was prepared in distilled water. The
photodegradation experiments were performed in a photoreactor made of quartz and
equipped with a specific tubular space for the UV lamp as well as a cooling jacket. A
high pressure mercury UV lamp (125 W) was placed at its specified position using a
special rod in the reactor. A continuous cold water (16±1°C) supply was maintained
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during the experiment to control the temperature of the reaction mixture. 350 ml of the
100 ppm MTBE stock solution previously prepared and the required amount of the
selected photocatalyst were stirred for 30 min to prepare a uniform dispersion of the ZnO
particles at room temperature followed by passage of oxygen current through an inlet
tube for 30 min at a moderate rate. After the specified time, the oxygen current was
ceased, and the UV lamp was turned on. The experimental setup was completely covered
with aluminum foil, and samples were collected every hour for a period of five hours for
analysis.
2.4. Characterization Techniques
The synthesized photocatalyst samples were characterized using advanced
instrumentation techniques. Scanning electron microscopy and transmission electron
microscopy of the samples were performed to determine the morphology and size of the
particles, and x-ray diffraction patterns were obtained using an X-ray diffractometer
equipped with a monochromatic high-intensity Cu K radiation (= 1.5418 Å, 40 kV, 100
mA).
The X-ray photoelectron spectroscopy (XPS) surface elemental analysis was conducted
using a Thermo ESCALAB 250 Xi with Al K Alpha radiation (1486.6 eV). The spectra
acquisition and processing were performed using the Thermo Avantage Software, version
4.58. The binding energy was referenced to the C1 s line at 284.6 eV for calibration. The
sample was introduced into the preparation chamber with the sample holder and degassed
until a good vacuum achieved. Then, the sample was transferred to the analysis chamber
where the vacuum was set to 10-9 – 10-10 mBar. The analyses were performed using the
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following parameters: Pass energy of 20 eV, Dwell time 50 ms and step size 0.1 eV. A
flood gun with a standard charge compensation mode was employed to neutralize the
charge build up on the surface of the insulating samples.
Nitrogen (N2) adsorption-desorption isotherms were determined at the liquid nitrogen
temperature (−195 ◦C) using an automatic ASAP 2010 Micromeritics sorptiometer
equipped with an outgassing platform and an on-line data acquisition and handling
system operating standard BET [34] and BJH [35] analytical software for the adsorption
data following the experimental recommendations previously reported [36]. The N2 gas
was 99.999% pure KOAC (Kuwait), and the test samples cerias (300 ± 2 mg) were pre-
outgassed at 110 ◦C and 10−5 Torr for 3 h. The reproducibility of the adsorption-
desorption isotherms was better than 95%.
3. Results and Discussion:
3.1. Electron Microscopy and X-ray Diffraction Studies
The morphology of the particles of the photocatalyst plays an important role in its
photoactivity. Therefore, the prepared photocatalysts were characterized by SEM and
TEM to study the shape and size of the 1% Pd doped ceria-ZnO. The morphology of
these particles observed by SEM is shown in Fig. 1, and these particles are round with a
uniform size distribution. The particles size of the 1% Pd doped ceria-ZnO are in the
range of 6-33 nm. The presence of Pd in the composites was not observed in the SEM
image of the sample, which might be due to the low amount of Pd doping. This result was
confirmed by TEM images, which are shown in Fig. 2. Two types of particles are clearly
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shown in the ceria-ZnO catalyst. Clear identification of the 1% Pd was not achieved due
to the small amount and high dispersion of the Pd over the composite oxide support.
Moreover Table 1 is showing atomic % of Pd in the samples investigated. In addition, the
EDX analysis that was conducted to semi-quantify the surface and near surface amount
of each element present. The Pd loading was confirmed by various methods including XPS,
EDX and the effect of Pd was clearly visible by the photocatalytic activity of the Pd supported
ceria-ZnO composite catalysts. However, EDX analysis of 1.0% Pd doped ceria-ZnO
indicated the presence of all of the components including Pd (Table 1, Fig. 3). The 1% Pd
doped ceria-ZnO sample was also analyzed with an XRD diffractometer. The crystalline
structure of the 1% Pd doped ceria-ZnO was characterized using a rotating-target X-ray
diffractometer (Japan Rigaku D/Max-2400) equipped with monochromatic high-intensity
Cu K radiation (= 1.5418 Å, 40 kV, 100 mA). The average crystalline size of the catalyst
nanoparticles was estimated from the full width half maximum (FWHM) and the peak
position of an XRD line broadened according the Scherrer formula [37]:
d = [0.9 λ /B cos θ] (1)
Where d is the average crystallite size, λ is the wavelength of the X-ray (0.15418 nm),
B is the full width at half maximum (FWHM, radian) and θ is the Bragg angle (degree).
The value of the FWHM was obtained by performing profile fitting using XRD pattern
processing software. The characteristic strong diffraction peaks obtained for the 1% Pd
doped ceria-ZnO composite catalysts are shown in Fig. 4. The characteristic peaks for Pd
were not observed in the diffractogram of the photocatalyst, which is most likely due to
the small amount of highly dispersed Pd present in the photocatalyst. The results of
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catalyst composition determined by EDX (Table 1) clearly show the amount of Pd loaded
is close to the nominal amount impregnated on ceria-ZnO photocatalysts. The XRD
spectrum peaks are summarized in Table 2 were a few of the peaks from the individual
components overlap with each other. All of the characteristic peaks are in good
agreement with those reported in the literature. Therefore, these results confirm the
existence presence of a ceria-ZnO composite system [31, 33]. The average crystallite size
of the 1% Pd doped ceria-ZnO was 20 nm. However, the characteristic peaks of the
individual oxide phase indicate that the ceria particles are much smaller in size
(approximately 6 nm) compared to the ZnO particles (20+ nm).
3.2. X-ray photoelectron spectroscopy and N2 Sorptiometry studies
Fig. 5 shows the Zn (2p), Ce (3d), Pd (3d), and O (1 s), XPS peaks of PCZ1.0. The peaks
were deconvoluted using standard software. Using the integrated peak areas and element
sensitivity factors, the total atomic percentage of the elements on the surface was
determined and reported in Table 3. The symmetry and binding energy of the Zn (2p)
peak confirm a +2 oxidation state. This oxidation state was further confirmed by
calculating the difference between the binding energies of the 2p3/2 and ep1/2 peaks,
which was determined to be 23.1 eV in good agreement with the literature values [28,
34]. The multi-peaks spectra (fundamental and satellite) of Ce (3d) are also shown in
Fig. 5. The relatively small peaks at 884.5 and 902.8 eV indicated a small amount of
Ce+3, and the pronounced peak at 916 eV confirmed that Ce+4 was the major species [39,
40]. The peaks at 337.1 and 342.3 eV in Fig. 5 correspond to Pd+2 [41]. Therefore the
XPS results confirm a structure consisting of Pd CeO2-x-ZnO with an atomic surface
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composition as reported in Table 3. Similar results (not presented) were found for
PCZ0.5 and PCZ1.5.
The N2 sorptiometry results are shown in Fig. 6 and Table 3. The isotherms of the
samples are type II and exhibited type H3 hysteresis (indicative of parallel plate or open
slits shape) [42]. The closure of the hysteresis at a low relative pressure for all of the
samples confirmed the wide pores, which are reported in Table 4 (18-27 nm). In
addition, the late and steep adsorption of N2 on the samples indicates a large pore size
and narrow pore size distribution [42]. Sample PCZ1.0 exhibits a lower specific surface
area (37 m2/g) and a larger pore size (27.1 nm). The hysteresis of sample PCZ1.0 was
determined to be the narrowest among the studied samples, which is due to its wider
pores. SBET SCfor PCZ1.0, and SBET < SC for PCZ0.5 and PCZ1.5. These results imply
that PCZ1.0 possesses cylindrical mesopores while the PCZ0.5 and PCZ1.5 samples
possess non-cylindrical mesopores [42]. The higher activity of sample PCZ1.0 may be
related to the pore size and shape.
3.3. Kinetic and Photodegradation Studies of MTBE in Water
The photocatalytic degradation of MTBE in water was studied by employing the ceria-
ZnO nanoparticles doped with 0.5% Pd, 1% Pd and 1.5% Pd as photocatalysts. The data
obtained from photocatalytic degradation of MTBE was plotted as degradation as a
function of time (Fig. 7). The 1% Pd doped ceria-ZnO nanoparticles exhibited the highest
photocatalytic activity compared to the other samples (i.e., 0.5% Pd doped and 1.5% Pd
doped ceria-ZnO). Nearly complete degradation of MTBE (99.6%) was observed with
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1% Pd doped ceria-ZnO after 5 hours compared to the other two catalysts 0.5% Pd doped
ceria-ZnO (90%) and 1.5% Pd doped ceria-ZnO (88.9). Therefore, the 1% Pd doped
ceria-ZnO nanoparticles with an optimum Pd loading are considered to be an effective
photocatalyst for the degradation of MTBE in water. Initially, the rate of the
photodegradation of MTBE was determined to be very fast, as shown in Fig. 7. After the
first hour of UV irradiation, the concentration of MTBE in the reaction medium was
determined to be 28.2 ppm for the ceria-ZnO nanoparticles doped with 1% Pd. The fast
photodegradation of MTBE in the first hour can be attributed to the presence of hydroxyl
radicals (•OH) whose concentration increases with UV irradiation and catalyst surface
area for adsorption of MTBE. However, as the reaction proceeds, photocatalytic
degradation of MTBE decreases due to the competition offered by the presence of other
species in the reaction medium for the hydroxyl radical and the adsorption surface. The
increased efficiency of the ceria-ZnO nanoparticles doped with 1% Pd is due to the fast
transfer of the photoexcited electrons from the surface of the semiconducting
photocatalyst to the noble metal, which acts as an electron reservoir [43-45]. Therefore,
the recombination of the photogenerated electrons and holes will be efficiently controlled
resulting in an increase in the photocatalytic activity of the catalyst [46, 47].
The enhancement of the photoactivity for different catalysts with the same pollutants is
not purely a function of BET surface area, and the presence of Nobel metals has a large
effect on the efficiency [48]. In our work, because the cumulative pore volume (Vp) was
determined to be similar for the three samples studied, the increase in photoactivity may
be related to the pore sizes and not the pore volumes (Table 4).
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It is known that the presence of a noble metal, (e.g., gold or palladium) on the surface of
a semiconducting metal oxide photocatalyst lowers the work function at the interface
with the adsorbed oxygen. Therefore, the electron transfer between the photocatalyst and
the adsorbed oxygen increases resulting in an increase in the number of peroxy/superoxy
species, which are highly oxidizing in nature, and an increase in the rate of the
photocatalytic reaction [49-53]. However, the concentration of the doped metallic
particles was also reported to affect the activity of the photo catalyst. For the ceria-ZnO
nanoparticles doped with 1.5% Pd, the activity of the catalyst decreased due to an
increase in the number of particles of the doped metal on the surface of the ceria-ZnO
nanoparticles resulting in a reduction in the adsorbed MTBE and less surface are
available for irradiation to initiate photoexcitation. The smaller pores in this sample (see
Table 4) may contribute to this lower adsorption tendency [53]. Therefore, the
photocatalytic activity of the catalyst decreased.
The heterogeneous photocatalysis is initiated by with the adsorption of organic
contaminant molecules onto the surface of the photocatalyst. These adsorbed contaminant
molecules react with hydroxyl radicals produced from the reaction between water and the
photogenerated electrons/holes generated in the photoexcitation process. The
heterogeneous photocatalytic degradation of the various pollutants in water follows the
Langmuir-Hinshelwood kinetic model [37, 38]. Therefore, the rate of the photocatalytic
degradation of the organic pollutants is proportional to the surface area coverage of the
photocatalyst by the organic pollutant molecules:
Rate (R) = - (dC/dT) α θ (2)
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= krθ = (krKC/1+KC), (3)
If KC<<1 and negligible
-ln(C/C0) = Kappt (4)
where θ, kr, K and C define the surface area covered, rate constant of the photocatalytic
degradation reaction, the adsorption coefficient of the reactant and the reactant
concentration, respectively. If the concentration (C) becomes very low, KC would be
negligible compared to 1. A plot of ln (C0/C) as a function of the irradiation time results
in a straight line representing a first order reaction. The rate constant of this reaction can
be obtained from the slope of the line in Fig. 8 [37]. The rate constant for the
photodegradation reaction increased as the percentage of Pd increased, and then, the rate
constant decreased after an optimum doping level was achieved. Fig. 8 shows that the 1%
Pd doped ceria-ZnO nanoparticles exhibit the highest rate constant (0.87 h-1), and the rate
constant obtained for 0.5% Pd and 1.5% Pd doped ceria-ZnO nanoparticles are 0.37 h-1
and 0.4 h-1, respectively.
4. Conclusions
Photocatalytic degradation of MTBE in water was evaluated using ceria-ZnO doped with
Pd as a photocatalyst. Nearly complete removal of MTBE was achieved within five hours
of UV irradiation using ceria-Z
nO nanoparticles doped with 1% Pd. The efficient
removal of MTBE is due to the higher concentration of hydroxyl radicals and the
presence of Pd, which controls the recombination of photogenerated electron hole pair. In
addition to the Pd loading, the N2 sorptiometry study introduced other factors that can
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affect the catalytic efficiency, such as the average catalyst pore sizes. The kinetics of the
photocatalytic degradation reaction of MTBE was observed to follow first order kinetics.
Acknowledgments: The authors wish to acknowledge the support by King Abdul Aziz
City for Science and Technology (KACST) through the Science & Technology Unit at
Umm Al-Qura University for funding from project No. 10-wat1240-10 as part of the
National Science, Technology and Innovation Plan. A. B. is acknowledges the support
provided through the general facilities projects GS01/01 and GS01/05 under the SAF
program of the Faculty of Science, Kuwait University.
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Figure Captions:
Fig. 1. SEM micrograph of 1% Pd doped ceria-ZnO.
Fig. 2. TEM image of the 1% Pd/ceria-ZnO photocatalyst.
Fig. 3. EDX spectra of the 1% Pd doped ceria-ZnO photocatalyst.
Fig. 4. XRD diffractogram of 1% Pd doped ceria-ZnO.
Fig. 5. Deconvoluted XPS peaks for Zn (2p), Ce (3d), Pd (3d) and O (1s) for the PCZ1.0
sample.
Fig. 6. N2 adsorption-desorption isotherms determined at -195 °C for the indicated
samples.
Fig. 7. Photocatalytic degradation of MTBE in water in the presence of the Pd doped
ceria-ZnO catalyst.
Fig. 8. Reaction kinetics of the photocatalytic degradation of MTBE in water in the
presence of the Pd doped ceria-ZnO catalyst.
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Table 1. Results of EDX analysis of Pd doped ceria-ZnO photocatalyst.
Elements (Weight %)
Sample O.K Zn K Pd K Ce K
PCZ0.5 14.25 71.54 0.40 13.81
PCZ1.0 14.15 71.01 1.06 13.78
PCZ1.5 15.04 69.93 1.43 13.60
Ceria-ZnO 25.48 60.58 NA 13.95
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Table 2. Details of XRD spectrum of 1% Pd doped ceria-ZnO photocatalyst.
S. No. Position 2θ (deg) Phase Name Size (nm)
1 28.70 Ceria, syn(1,1,1) 5.8
2 31.89 Zinc Oxide(1,0,0) 23.3
3 34.47 Zinc Oxide(0,0,2) 32.9
4 36.33 Zinc Oxide(1,0,1) 22.1
5 47.68 Zinc Oxide(1,0,2),Ceria,
syn(2,2,0)
10.4
6 56.67 Zinc Oxide(1,1,0),Ceria,
syn(3,1,1)
20.3
7 62.98 Zinc Oxide(1,0,3) 19.3
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Table 3. XPS-determined photoelectron binding energies (BE/±0.5 eV) and surface
atomic % of the studied samples.
Sample Zn 2p Ce 3d Pd 3d O 1s
PCZ0.5 37.6 6.7 0.4 48.8
PCZ1.0 39.6 8.5 0.7 50.3
PCZ1.5 37.6 5.9 0.6 50.3
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Table 4. Surface characteristics of the catalysts. BET-specific surface area (SBET ±2
m2/g), BJH-cumulative surface area (SC ±3 m2/g), BJH-average cumulative pore volume
(VpC ± 0.002 cm3/g) and pore diameter (dp ± 0.2 nm).
Catalyst SBET SC VpC dp
PCZ0.5 47 57 0.260 18.4
PCZ1.0 37 41 0.279 27.1
PCZ1.5 49 58 0.293 20.3
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Graphical Abstract
To create your abstract, type over the instructions in the template box below.Fonts or abstract dimensions should not be changed or altered.
Preparation and characterization of Pd doped
ceria-ZnO nanocomposite catalyst for
methyl tert-butyl ether (MTBE) photodegradation
Zaki S. Seddigi, Ali Bumajdad, Shahid P. Ansari, Saleh A. Ahmed,
Ekram Danish, Naeema H. Yarkandi and Shakeel Ahmed
Leave this area blank for abstract info.
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Highlights
Novel Pd supported ceria-ZnO photocatalysts were prepared with different
amounts of palladium.
The photocatalytic activity of these catalysts was evaluated for degradation of
MTBE in water.
Near complete removal of MTBE was achieved using 1% Pd doped ceria-ZnO
catalyst and UV irradiation.
Highest rate constant was obtained in case of 1% Pd doped ceria-ZnO
catalyst.
Shape and size of pores are important factors for high photoactivity of
catalyst.
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List of figures
Figure 1
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Figure 2
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Figure 3
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Figure 4
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Figure 5
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Figure 6
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Figure 7
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Figure 8