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www.elsevier.com/locate/apcatb
Applied Catalysis B: Environmental 56 (2005) 305–312
Photocatalytic degradation of phenol on MWNT and titania composite
catalysts prepared by a modified sol–gel method
Wendong Wanga, Philippe Serpb, Philippe Kalckb, Joaquim Luıs Fariaa,*
aLaboratorio de Catalise e Materiais, Departamento de Engenharia Quımica, Faculdade de Engenharia da Universidade do Porto,
Rua Dr. Roberto Frias s/n, 4200-465 Porto, PortugalbLaboratoire de Catalyse, Chimie Fine et Polymeres, Ecole Nationale Superieure d’Ingenieurs en Arts Chimiques et Technologiques,
118 Route de Narbonne, Toulouse Cedex 31077, France
Received 26 May 2004; received in revised form 28 September 2004; accepted 29 September 2004
Available online 11 November 2004
Abstract
Multi-walled carbon nanotubes (MWNT) and nanocrystalline titania composite catalysts were prepared by a modified sol–gel method.
Thermogravimetric analysis, N2 adsorption–desorption isotherm measurements, powder X-ray diffraction, scanning electron microscopy,
energy dispersive X-ray analysis, transmission electron microscopy and UV–vis spectra were carried out to characterize the composite
catalysts with different MWNT contents. The results suggest that the presence of MWNT embedding in the composite catalysts matrix
prevents TiO2 particle agglomeration. Additionally, a correlation exists between the MWNT content and the changes in the UV–vis absorption
properties. The photocatalytic degradation of phenol was chosen as a model reaction to evaluate the photocatalytic activities of the composite
catalysts. An optimum of the synergetic effect was found for a weight ratio MWNT/TiO2 equal to 20%. The effects induced by MWNT on the
composite catalysts may be explained in terms of a strong interphase interaction between MWNT and TiO2 in the composite catalysts.
# 2004 Elsevier B.V. All rights reserved.
Keywords: Photocatalysis; Phenol degradation; Titanium dioxide; MWNT; Composite catalyst
1. Introduction
Titanium dioxide has been extensively employed as
photocatalytic material for solving environmental problems,
especially for eliminating toxic chemicals from wastewater
[1,2]. Anatase crystalline form of titania has been found to
be the most active photocatalyst. TiO2/UV system has been
widely investigated in the heterogeneous photocatalytic
process, during which UV irradiation upon the semicon-
ductor can photo-activate the TiO2 active centers to give
electron/hole (e�/h+) couples. Oxygen is often present as the
electron acceptor to form the superoxide radical ion (O2��),
while OH� and H2O are available as electron donors to yield
the hydroxyl radical (HO�); both of which are very reactive
and strongly oxidizing to be capable of totally mineralizing
organic pollutants [3].
* Corresponding author. Tel.: +351 225 081 645; fax: +351 225 081 449.
E-mail address: [email protected] (J.L. Faria).
0926-3373/$ – see front matter # 2004 Elsevier B.V. All rights reserved.
doi:10.1016/j.apcatb.2004.09.018
The photocatalytic activities of TiO2 powder greatly
depend upon its microstructure and physical properties.
Many studies [4–12] have investigated the relationship
between the conditions and methods of synthesis and the
properties of the resulting TiO2, such as surface area, particle
size, pore volume and pore size distribution, crystal structure
and crystallinity, phase composition, thermal stability,
bandgap energy, among others. Within the synthesis
methods, the sol–gel technique from alkoxide precursors
is one of the most used. It provides a versatile synthetic route
in which the operation conditions and variables, including
different solvent removal procedures [6], surfactant or
polymer modification [10], UV illumination [11] and
ultrasonication [12], can be adjusted to produce anatase
TiO2 with tailored morphological features.
It has been reported that activated carbon (AC) have
some beneficial effects on the photocatalytic activity of TiO2
[13–16]. Different preparation methods have been used to
introduce carbon into the TiO2 and activated carbon system,
W. Wang et al. / Applied Catalysis B: Environmental 56 (2005) 305–312306
such as mixing TiO2 with activated carbon [13,14,17],
precipitating TiO2 onto the surface of activated carbon
[15,16] and polymerizing a mixture of resorcinol, for-
maldehyde and titanium precursor [18,19].
In a recent review, attention has been called to the fact
that carbon nanotubes (CNT) are attractive and competitive
catalyst supports when compared to activated carbon due to
the combination of their electronic, adsorption, mechanical
and thermal properties [20]. Some recent works have
emphasized on the preparation of new hybrid materials
CNT–TiO2. A sol–gel method has been used to prepare the
inclusion of CNT into an inorganic film of TiO2 matrix [21].
Multi-walled carbon nanotubes-based titania composite
material has been prepared by an impregnation method
[22], which provides a homogeneous inorganic cover layer
on the surface of purified MWNT. Rutile TiO2 has been
immobilized on the sidewall of MWNT by a simple one-step
scheme, which produces three distinct morphologies of
hybrid MWNT at different reaction temperatures [23].
Coating MWNT surface with TiO2 has been performed by a
sol–gel method using different alkoxides and by hydro-
thermal hydrolysis of TiOSO4, which can lead to different
morphologies [24].
Composites containing carbon nanotubes are believed to
provide many applications and exhibit cooperative or
synergetic effects between the metal oxides and carbon
phases. In the case of TiO2, the only reported study on this
matter failed to confirm this prediction [25] and in the
present work, we focus on the preparation and characteriza-
tion of MWNT–TiO2 composite catalysts using a modified
acid-catalyzed sol–gel method. The unique properties of
MWNT are utilized to optimize the surface and catalytic
properties of MWNT–TiO2 composite catalysts, and phenol
is used as a probe molecule to evaluate the photocatalytic
properties of the composite catalysts.
2. Experimental
2.1. Catalysts preparation
High-purity MWNT were synthesized by a catalytic
chemical vapour deposition (CCVD) method in fluidized
bed reactor on a Fe/Al2O3 catalyst [26], and their
purification was achieved according to a standard sulphuric
acid washing procedure. The mean external and internal
diameters of the nanotubes are 17 and 8 nm, respectively,
and their length is of several micrometers.
MWNT–TiO2 composite catalysts were prepared by
means of a modified acid-catalyzed sol–gel method from
alkoxide precursors. The preparation was performed at room
temperature as following: 0.1 mol of Ti(OC3H7)4 (Aldrich
97%) was dissolved in 200 mL of ethyl alcohol. The solution
was stirred magnetically for 30 min, and then 1.56 mL of
nitric acid (65 wt.%) was added. Subsequently, certain
amount of MWNT was introduced into the Ti(OC3H7)4
ethanol solution. The mixture was loosely covered and kept
stirring until a homogenous MWNT-contained gel formed.
The gel was aged in air for 1 week. Then, the xerogel was
grinded into a fine powder and dried at room temperature.
The powder was calcined at 400 8C in a flow of nitrogen for
2 h to obtain MWNT–TiO2 composite catalysts. Catalysts
are named as X-MWNT–TiO2, where X (1, 5, 10, 20 and 40)
corresponds to the weight ratio of MWNT to a 100 weight
basis of neat TiO2 (ex. 20-MWNT–TiO2 means
20(MWNT):100(TiO2), w/w).
2.2. Characterization methods
Thermogravimetric (TG) and differential thermogravi-
metric (DTG) analysis of the xerogels were performed in a
flow of nitrogen with a Mettler TA 4000 system from 25 to
800 8C at a heating rate of 10 8C/min. The amount of carbon
in the composite catalysts was estimated from weight loss in
air by using the same conditions.
N2 adsorption–desorption isotherm measurements were
carried out at 77 K using an Omnisorp 100 CX apparatus.
Specific surface area determinations were evaluated in the
equilibrium points p/p0 range from 0.05 to 0.25 by BET
method.
Powder X-ray diffraction (XRD) patterns were recorded in
the range 2u = 20–608 on a Philips X’Pert MPD rotatory target
diffractometer, using Cu Ka radiation (l = 0.15406 nm) as X-
ray source, operated at 40 kV and 50 mA. Crystallite size of
anatase TiO2 can be determined from the line broadening by
using Scherrer’s formula.
Scanning electron microscopy (SEM) was carried out in a
Jeol JSM-6301F instrument, which was equipped with an
energy dispersive X-ray (EDX) detector.
Transmission electron microscopy (TEM) observations
were made with a Phillips CM12 electron microscope
(120 kV voltage). The samples were dispersed in ethanol,
sonicated and collected on a copper carbon-coated TEM
grid.
The UV–vis spectra of the solid powder materials were
measured on a JASCO V-560 UV–vis spectrophotometer,
equipped with an integrating sphere attachment (JASCO
ISV-469). The powder was not diluted in any matrix to avoid
a decrease of the absorbance. The spectra were recorded in
diffuse reflectance mode and transformed by the instrument
software (JASCO) to equivalent absorption Kubelka-Munk
units.
2.3. Photoreactor and photodegradation experiments
The experiments were carried out in a glass immersion
photochemical reactor charged with 800 mL of aqueous
solution/suspension. The reactor was equipped with a UV
lamp, located axially and held in a quartz immersion. The
UV radiation source is a Heraeus TNN 15/32 low-pressure
mercury vapor lamp (3 W of the radiant flux). The solution/
suspension was magnetically stirred. A typical irradiation
W. Wang et al. / Applied Catalysis B: Environmental 56 (2005) 305–312 307
Fig. 1. Thermogravimetric analysis of (a) 20-MWNT–TiO2 xerogel in N2
and (b) 20-MWNT–TiO2 composite catalyst in air.
was performed in open air with continuous stirring, which
proved to supply enough oxygen for oxidation photode-
gradation. In case of need, there was a feeding system
connected to the reactor for bubbling through the solution/
suspension a controlled flow of oxygen at different partial
pressures.
The initial phenol concentration (C00) was 50 mg/L. TiO2
concentration was 1 g/L and the amount of carbon was
considered for the different composite catalysts. Before
illumination was turned on, the suspension with phenol and
photocatalyst was magnetically stirred in a dark condition
for 60 min to establish an adsorption–desorption equili-
brium. The suspension was irradiated under UV light with
constant stirring speed during the photoreaction process.
The first sample was taken out at the end of the dark
adsorption period, just before the light was turned on, in
order to determine the phenol concentration in solution,
which was hereafter considered as the initial concentration
(C0) after dark adsorption. Samples were then withdrawn
regularly from the reactor and centrifuged immediately for
separation of the suspended solids. The clean transparent
solution was analyzed with UV–vis spectroscopy as
described as following.
The UV–vis spectrum of the phenol solution was
recorded on the same JASCO V-560 UV–vis spectro-
photometer, equipped with a double monochromator and
double beam optical system. The full spectrum (200–
800 nm) of each sample was recorded and the absorbance at
selected wavelength (270 nm) was registered to determine
the phenol concentration. In order to minimize inaccuracy
due to the occurrence of other oxidation products that may
absorb at the same wavelength, the residual absorbance
measured after 6 h reactions was determined carefully, but
found to be negligible when compared to the error of the
method. Additionally, no isobestic points were visible when
the set of full spectra of the samples taken at different times
was analyzed, therefore ruling out the possibility of
significant interference by any intermediate at the wave-
length of analysis. Repetition tests were made to ensure the
reproducibility. For the purpose of kinetic analysis, each
sample taken from the reactor was divided into three vials
and the final absorption was given by the arithmetic average
over three measurements.
3. Results and discussion
3.1. Catalyst characterization
The thermal behavior of the xerogel was investigated in
order to evaluate the stability of the prepared composites.
Fig. 1a shows the typical evolution of 20-MWNT–TiO2
xerogel during calcination in nitrogen up to 800 8C. Other
samples with different initial amounts of MWNT showed
similar evolution profiles. DTG curve presents one intense
band at 69 8C and one broad band at 202 8C, which can be
attributed to the evaporation of alcohol solvent and the
decomposition of TiO2 precursor during TiO2 crystallization
process, respectively. TG curve indicates mass loss up to
400 8C of a total 29%, followed by less than 2% loss up to
800 8C. The evolution of 20-MWNT–TiO2 composite
catalyst during calcination in air is shown in Fig. 1b. TG
curves show three different steps for the weight loss. Initially
a weak endothermic effect due to water removal and
structural water evolution (i.e. OH groups), followed by a
steep decrease in mass due to MWNT oxidation, and finally
a very slow loss up to 800 8C. DTG curve features only one
intense band centered at 493 8C, which corresponds to the
disappearance of MWNT. We have measured a maximum
gasification rate at around 554 8C for neat MWNT under the
same experimental conditions (not shown). The difference in
the thermal stability of MWNT can be attributed to the
presence of TiO2 in the composite catalysts, which might
catalyze carbon gasification and lower the temperature at
which the maximum gasification rate occurs. The TiO2
phase is quite stable at this temperature range, as inferred by
the analysis of the corresponding TG profile (not shown)
where no mass loss is observable. For the 20-MWNT–TiO2,
the carbon content estimated from the TG curves is 16.4%.
The carbon contents of the other composite catalysts with
different initial amounts of MWNT are also listed in Table 1.
As expected, since the materials were calcined at 400 8C in a
W. Wang et al. / Applied Catalysis B: Environmental 56 (2005) 305–312308
Table 1
Carbon content calculated from initial ratios (Ccal) and determined by TG
(CTG), BET surface area and TiO2 crystal size (dTiO2) of the MWNT–TiO2
composite catalysts compared to the base components
Catalyst Ccal (wt.%) CTG (wt.%) BET (m2/g) dTiO2(nm)
1-MWNT–TiO2 1.0 1.0 111 8.1
5-MWNT–TiO2 4.8 4.6 114 7.9
10-MWNT–TiO2 9.1 8.8 124 7.7
20-MWNT–TiO2 16.7 16.4 139 7.4
40-MWNT–TiO2 28.6 27.1 163 6.4
TiO2 0 – 107 8.5
MWNT 100 – 169 –
flow of nitrogen for 2 h, there is no appreciable degradation
of the MWNT and the determined carbon content (CTG)
agrees very well with the calculated from the initial ratios
(Ccal).
The N2 adsorption–desorption isotherms for TiO2, neat
MWNT, and MWNT–TiO2 composites were taken for
characterization purposes of the surface areas. The isotherm
of MWNT is identical with the reported ones, where pores in
MWNT can be mainly divided into inner hollow cavities of
small diameter and aggregated pores formed by interaction of
isolated MWNT [27]. All the plots of the composite catalysts
(only 20-MWNT–TiO2 shown in Fig. 2) can be ascribed to
type IV isotherms according to IUPAC classification, which
confirm that a mesoporous pore texture of the nanotubes can
be preserved after the introduction of TiO2.
In Table 1, the results from BET surface area
measurements for the composite catalysts are also given.
The surface areas of neat TiO2 and MWNT are 107 and
169 m2/g, respectively, while those of composite catalysts
vary from 111 to 163 m2/g, increasing with the initial
MWNT/TiO2 ratios from 1 to 40%. It is interesting to note
that the surface areas of composite catalysts are higher than
those estimated theoretically in proportion to the TiO2 and
MWNT contents. Overall there is a decrease of the surface
area when compared to that of the neat MWNT, which is in
line with previous observations [16]. It is expected that the
introduction of TiO2 onto various activated carbons results
in certain reduction of specific surface area. On the other
hand, the present approach is quite the opposite, since here
the MWNT are being introduced in a TiO2 matrix, thus
increasing the surface area of the neat titania. The fact that
this increase leads to surface area higher than expected
means that there must be a strong structural effect between
the carbon and metal oxide phases.
In order to investigate this effect, the XRD patterns of
neat MWNT, TiO2 and MWNT–TiO2 composite catalysts
with different MWNT content are compared in Fig. 3. The
most intense two peaks of MWNT correspond to the (0 0 2)
and (1 0 0) reflections, respectively. Only TiO2 in anatase
Fig. 2. N2 adsorption–desorption isotherm of 20-MWNT–TiO2.
phase can be indexed from the patterns for TiO2 and
composite catalysts. The rutile and brookite phases of TiO2
are not observed. It is noteworthy that the characteristic
peaks of MWNT can hardly been identified from the patterns
of composite catalysts. Although the most intense peaks of
MWNT corresponding to (0 0 2) reflection overlaps the
anatase (1 0 1) reflection, all the composite catalysts present
symmetric peak of anatase (1 0 1) reflection in their
diffraction patterns. Additionally, the other intense peak
of MWNT due to (1 0 0) reflection between 408 and 458,where no peak can be attributed to TiO2, is also absent for all
the composite catalysts, even for 40-MWNT–TiO2 with the
highest MWNT content. However, it is not expected that the
crystal structure of MWNT may undergo great damage
during the present relatively mild preparation process. It is
observed that the peaks width broaden slightly but gradually
with the increase of MWNT content for the composite
catalysts. Crystallite sizes estimated from the line broad-
ening of anatase TiO2 (2 0 0) reflection plane (2u = 48.18),where there is hardly any interference from MWNT, are
listed in Table 1. The neat TiO2 of 8.5 nm size is obtained,
while the crystallite sizes of composite catalysts decrease
gradually from 8.1 to 6.4 nm from sample 1-MWNT–TiO2
to 40-MWNT–TiO2. This result is consistent with the
increasing MWNT/TiO2 ratios from 1 to 40%, which favors
Fig. 3. X-ray diffraction patterns of (a) MWNT, (b) TiO2, (c) 1-MWNT–
TiO2, (d) 5-MWNT–TiO2, (e) 10-MWNT–TiO2, (f) 20-MWNT–TiO2 and
(g) 40-MWNT–TiO2.
W. Wang et al. / Applied Catalysis B: Environmental 56 (2005) 305–312 309
Fig. 4. EDX spectrum of 20-MWNT–TiO2.
Fig. 5. SEM micrographs of MWNT and TiO2 composite catalysts (a) 5-
MWNT–TiO2 and (b) 20-MWNT–TiO2.
less extended crystallized TiO2 domains on MWNT surface
and thus avoiding TiO2 particles agglomeration.
EDX analyses were carried out to confirm the presence of
MWNT embedding in TiO2 matrix. Typically, the EDX
spectrum of 20-MWNT–TiO2 is presented in Fig. 4, which
expressly confirms the presence of C, O and Ti. The spectra
of other composite catalysts indicate different intensity of
peaks assigned to C due to different MWNT content.
The morphologies of MWNT and TiO2 composite
catalysts with different MWNT contents were revealed by
SEM investigation and SEM images of 5-MWNT–TiO2 and
20-MWNT–TiO2 are shown in Fig. 5. For the composite
catalyst with low MWNT content at 5%, MWNT-embedded
TiO2 and separated TiO2 particles can be identified, while
those with higher MWNT content feature relatively
homogeneous MWNT embedding in TiO2 matrix without
apparent agglomeration of TiO2 particles.
Representatively, TEM images of 20-MWNT–TiO2
composite catalyst are shown in Fig. 6. The low-
magnification image presents an overall view of MWNT,
with external diameters ranging from 15 to 20 nm,
embedding in TiO2 matrix. The inset in Fig. 6a reveals
typically TiO2 nanoparticles on MWNT surface, which is
Fig. 6. TEM images of 20-MWNT–TiO2: (a) overall view of MWNT
embedding in TiO2 matrix and in inset MWNT surface covered with
TiO2 nanoparticles; (b) TiO2 nanoparticle on MWNT surface with a higher
magnification.
W. Wang et al. / Applied Catalysis B: Environmental 56 (2005) 305–312310
Fig. 8. Kinetics of phenol removal under UV illumination in the presence of
various solids (the vertical line at time 0 isolates the dark adsorption period
from that under UV illumination).
observed more explicitly in the image with high magnifica-
tion (Fig. 6b). The average particle size of TiO2 determined
from the TEM images for 20-MWNT–TiO2 is about 7.5 nm,
which is consistent with those calculated from the XRD peak
broadening.
The diffuse reflectance UV–vis spectra of the composite
catalysts, expressed in terms of Kubelka-Munk equivalent
absorption units, are presented in Fig. 7. As expected neat
TiO2 has no absorption above its fundamental absorption
sharp edge rising at 400 nm. On the other hand, the
composite catalysts with MWNT can absorb at higher
wavelengths than that of TiO2. An apparent enhancement of
absorption is observed even for the composite catalyst with
1% MWNT content, and the absorption is totally over the
whole range of the UV–vis spectrum for 40-MWNT–TiO2.
It is noticeable that there is an obvious correlation between
the MWNT content and the UV–vis spectrum change. The
enhancements of absorption increase with the increase in
MWNT content of the composite catalyst. These results are
quite different from those of the activated carbon and TiO2
systems [14,17], where there is no correlation between the
activated carbon content and the UV–vis spectrum change.
These observations may indicate an increment of surface
electric charge of the oxides in composite catalysts due to
the introduction of MWNT.
3.2. Photocatalytic degradation of phenol
Kinetics plots correspond to phenol removal from its
aqueous solution by MWNT, TiO2 and their composite
catalyst are plotted against UV irradiation time in Fig. 8. It
can be observed that phenol decomposition in the presence
of MWNT, as well as the direct photolysis without any solid,
is negligible with less than 5% conversion within 4 h UV
irradiation. Complete disappearance of phenol (more than
95% of conversion) is observed in about 6 h of UV
irradiation for neat TiO2. Similar results are obtained on
commercially available TiO2 P25 under the same reaction
Fig. 7. UV–vis spectra of (a) TiO2, (b) 1-MWNT–TiO2, (c) 5-MWNT–
TiO2, (d) 10-MWNT–TiO2, (e) 20-MWNT–TiO2 and (f) 40-MWNT–TiO2.
condition, which can also be referred elsewhere [13,28]
despite different experimental systems. The introduction of
MWNT into TiO2 by a modified sol–gel method remarkably
induces a kinetic synergetic effect on phenol disappearance.
The complete elimination of phenol from the solution on the
irradiated composite catalyst 20-MWNT–TiO2 can be
achieved within 4 h. By contrast, phenol conversions after
4 h of irradiation are listed in Table 2 for each catalyst to
evaluate their activities, and neat TiO2 can only reach 44.2%
of phenol conversion within the same reaction time.
The influence of MWNT loading upon the conversion of
phenol disappearance has been followed in Fig. 9. An
optimum of the synergetic effect is found for 20-MWNT–
TiO2 with a weight ratio MWNT/TiO2 equal to 20%. The
increase of weight ratio MWNT/TiO2 from 1 to 20% favors
the synergetic effect on phenol disappearance, which
indicates the increase of phenol conversions after 4 h of
irradiation from 46.2 to 97.3% (Table 2). The decrease in
activity with higher MWNT/TiO2 weight ratio is considered
to be related to increased absorbing and scattering of
photons by carbon in the photoreaction system.
A suspended mechanical mixture of 20% MWNT and
TiO2 was prepared by merely stirring and its photocatalytic
behaviour is compared with neat TiO2 and 20-MWNT–TiO2
Table 2
Summary of phenol conversion upon 4 h irradiation (X4 h, %) and phenol
concentration after 1 h dark adsorption (C0, mg/L) on different solids for a
given initial concentration of phenol at 50 mg/L
Catalyst C0 (mg/L) X4 h (%)
1-MWNT–TiO2 47.3 46.2
5-MWNT–TiO2 47.2 73.5
10-MWNT–TiO2 46.3 81.0
20-MWNT–TiO2 45.9 97.3
40-MWNT–TiO2 45.4 87.1
TiO2 47.9 44.2
MWNT 46.9 4.9
20%MWNT + TiO2 46.5 61.5
W. Wang et al. / Applied Catalysis B: Environmental 56 (2005) 305–312 311
Fig. 9. Conversion of phenol photodegradation for MWNT and TiO2
composite catalysts with different MWNT contents.
composite catalyst in Fig. 10. As expected, the irradiated
mechanic mixture shows less synergetic effect than the
composite catalyst with the same MWNT content and
completely eliminates phenol from the solution within 6 h.
In order to explain the synergetic effect of CNT on the
activity of the composite catalysts, several reasons can be
evoked. The first explanation is purely physical and can be
described in terms of MWNT acting as dispersing agent
preventing TiO2 from agglomerating, thus providing a high
active surface area of the resulting composite catalyst.
Additionally, the effect induced by MWNT on the composite
catalysts can also be explained in terms of two different
mechanisms: either by acting as adsorbent or as photo-
sensitizer. In the case of the first mechanism, phenol adsorbs
on the carbon nanotubes, then by a transfer of the compound
to TiO2 surface, where it undergoes the photocatalytic
degradation [13,14,29]. The driving force for this transfer is
probably the difference in the phenol concentration between
MWNT and TiO2, which may cause surface diffusion of the
organic compound from MWNT to TiO2. The latter suggests
Fig. 10. Conversion of phenol photodegradation for MWNT and TiO2
composite catalyst and mechanical mixture with the same MWNT content.
that carbon nanotubes may act as photosensitizer by
injecting electrons into the TiO2 conduction band and
triggering the photocatalytic formation of very reactive
radicals (e.g. superoxide radical ion O2�� and hydroxyl
radical HO�), which is responsible for the degradation of the
organic compound [14,30].
It is noticeable that the increase in phenol conversion
(Table 2) follows in first approximation the decrease in TiO2
particle size (Table 1), thus the increase in active surface
area, when increasing MWNT/TiO2 ratio. However, there is
a limit to this correspondence since it is observed a decrease
in conversion over 20-MWNT–TiO2. This indicates that the
effect of activity increase due to increase in MWNT loading
is weighed down by photon absorbing and scattering by the
carbon phase, although higher MWNT loading can enhance
the dispersion of TiO2 particles. Being so, the role of MWNT
as a dispersing agent is not likely to be the most important
one accounting for the observed synergetic effect.
From Table 2, it is also noticed that all the solids show
comparable phenol concentration after 60 min dark adsorp-
tion period, which indicates similar adsorption capacities for
different solids. This result is different from the adsorption
behaviour in a TiO2 and activated carbon system [13,16]. In
the case of a mechanical mixture of TiO2 and activated
carbon, the adsorption constant of phenol on the mixture are
two orders of magnitude than that on neat TiO2, and more
than 60% phenol in the solution was adsorbed after 1 h dark
adsorption period for the mixture while less than 10% for
neat TiO2 [13]. Moreover, the removal of phenol was as high
as about 80% in the first 1 h reaction for a TiO2-mounted
activated carbon system, which was reasonably supposed to
be caused mainly by phenol adsorption [16].
With respect to the MWNT and TiO2 composite catalysts
in the present work, the phenol concentrations decrease by
less than 10% for all the solids after 60 min dark adsorption
period, and the introduction of MWNT into the composite
catalysts does not provide an apparently additive effect on
their adsorption capacities. Therefore, it is more reasonable
to believe that the synergetic effect on the removal of phenol
could be ascribed to MWNT acting as photosensitizer
instead of acting as adsorbent in the composite catalysts.
Furthermore, the composite catalyst prepared by the sol–gel
method demonstrates higher photocatalytic activity than the
mechanic mixture with the same MWNT content due to
MWNT embedded in the TiO2 matrix in the composite
catalyst, which can result in an intimate contact between
MWNT and TiO2 phases. This result suggests that a stronger
interphase interaction may be triggered between these two
phases in the composite catalyst than in the mixture.
4. Conclusions
MWNT–TiO2 composite catalysts have been prepared by
a modified sol–gel method. MWNT in the composite
catalysts indicate modified thermal and adsorption proper-
W. Wang et al. / Applied Catalysis B: Environmental 56 (2005) 305–312312
ties in comparison to neat MWNT. On the other hand, the
presence of MWNT in the composite catalysts can be
embedded in the TiO2 matrix and mitigate the agglomera-
tion of TiO2 particles, so as to increase the surface area of the
composite catalysts. UV–vis spectra of the solids indicate
that the enhancements of absorption increase with the
increase in MWNT/TiO2 ratio from 1 to 40% of the
composite catalyst. Synergetic effects have been observed
for the MWNT–TiO2 composite catalysts on the photo-
catalytic degradation of phenol. The increase of MWNT/
TiO2 ratio from 1 to 20% favors the enhancement of the
synergetic effect on phenol disappearance, although the
composite catalysts with different MWNT content show
comparable phenol adsorption capacities during dark
adsorption period. Higher photocatalytic activity is observed
in case of the composite catalyst prepared by the sol–gel
method in comparison to an MWNT and TiO2 mixture with
the same MWNT content. The results can be explained in
terms of the intimate contact between MWNT and TiO2
phases, which suggests that a strong interphase interaction
may be triggered between these two phases and MWNT
might behave as photosensitizer in the composite catalysts.
Acknowledgements
This work was supported by Fundacao para a Ciencia e a
Tecnologia, POCTI and FEDER (projects SFRH/BPD/
11598/2002 and POCTI/118/2003) and by CRUP (F-12/03).
Thanks to Conference des Presidents d’Universite for
financial support ‘‘Action integree Luso-Francaise’’.
References
[1] A. Fujishima, T.N. Rao, D.A. Tryk, J. Photochem. Photobiol. C 1
(2000) 1.
[2] A. Mills, S.L. Hunte, J. Photochem. Photobiol. A 108 (1997) 1.
[3] O.M. Alfano, M.I. Cabrera, A.E. Cassano, J. Catal. 172 (1997) 370.
[4] Z. Zhang, C.-C. Wang, R. Zakaria, J.Y. Ying, J. Phys. Chem. B 102
(1998) 10871.
[5] G. Colon, M.C. Hidalgo, J.A. Navio, Catal. Today 76 (2002) 91.
[6] T. Boiadjieva, G. Cappelletti, S. Ardizzone, S. Rondinini, A. Vertova,
Phys. Chem. Chem. Phys. 5 (2003) 1689.
[7] K.Y. Jung, S.B. Park, S.-K. Ihm, Appl. Catal. A 224 (2002) 229.
[8] B. Li, X. Wang, M. Yan, L. Li, Mater. Chem. Phys. 78 (2002) 184.
[9] M. Hirasawa, T. Seto, T. Orii, N. Aya, H. Shimura, Appl. Surf. Sci.
197–198 (2002) 661.
[10] M.M. Yusuf, Y. Chimoto, H. Imai, H. Hirashima, J. Sol–Gel Sci.
Technol. 26 (2003) 635.
[11] H. Liu, W. Yang, Y. Ma, Y. Cao, J. Yao, J. Zhang, T. Hu, Langmuir 19
(2003) 3001.
[12] P.S. Awati, S.V. Awate, P.P. Shah, V. Ramaswamy, Catal. Commun. 4
(2003) 393.
[13] J. Matos, J. Laine, J.-M. Herrmann, Appl. Catal. B 18 (1998) 281.
[14] C.G. Silva, J.L. Faria, J. Photochem. Photobiol. A 155 (2003) 133.
[15] G. Colon, M.C. Hidalgo, M. Macias, J.A. Navio, J.M. Dona, Appl.
Catal. B 43 (2003) 163.
[16] B. Tryba, A.W. Morawski, M. Inagaki, Appl. Catal. B 41 (2003) 427.
[17] J. Arana, J.M. Dona-Rodriguez, E.T. Rendon, C.G.I. Cabo, O. Gon-
zalez-Diaz, J.A. Herrera-Melian, J. Perez-Pena, G. Colon, J.A. Navio,
Appl. Catal. B 44 (2003) 161.
[18] F.J. Maldonado-Hodar, C. Moreno-Castilla, J. Rivera-Utrilla, Appl.
Catal. A 203 (2000) 151.
[19] C. Moreno-Castilla, F.J. Maldonado-Hodar, F. Carrasco-Marin, E.
Rodriguez-Castellon, Langmuir 18 (2002) 2295.
[20] P. Serp, M. Corrias, P. Kalck, Appl. Catal. A 253 (2003) 337.
[21] P. Vincent, A. Brioude, C. Journet, S. Rabaste, S.T. Purcell, J.L. Brusq,
J.C. Plenet, J. Non-Cryst. Solids 311 (2002) 130.
[22] K. Hernadi, E. Ljubovic, J.W. Seo, L. Forro, Acta Mater. 51 (2003)
1447.
[23] Q. Huang, L. Gao, J. Mater. Chem. 13 (2003) 1517.
[24] A. Jitianu, T. Cacciaguerra, R. Benoit, S. Delpeux, F. Beguin, S.
Bonnamy, Carbon 42 (2004) 1147.
[25] J. Sun, L. Gao, Carbon 41 (2003) 1063.
[26] M. Corrias, B. Caussat, A. Ayral, J. Durand, Y. Kihn, P. Kalck, P. Serp,
Chem. Eng. Sci. 58 (2003) 4475.
[27] Q.-H. Yang, P.-X. Hou, S. Bai, M.-Z. Wang, H.-M. Cheng, Chem.
Phys. Lett. 345 (2001) 18.
[28] B. Tryba, A.W. Morawski, M. Inagaki, Appl. Catal. B 46 (2003) 203.
[29] J. Matos, J. Laine, J.-M. Herrmann, J. Catal. 200 (2001) 10.
[30] C. Lettmann, K. Hildenbrand, H. Kisch, W. Macyk, W.F. Maier, Appl.
Catal. B 32 (2001) 215.