Journal of Water Process Engineering 20 (2017) 71–77
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Journal of Water Process Engineering
journal homepage: www.elsevier.com/locate/jwpe
Photocatalytic degradation of a model textile dye using Carbon-doped
titanium dioxide and visible light
MARK
Giuseppe Cinellia,1, Francesca Cuomoa,1, Luigi Ambrosoneb, Matilde Colellac, Andrea Cegliea,
⁎
⁎
Francesco Vendittia, , Francesco Lopeza,
a
Department of Agricultural, Environmental and Food Sciences (DiAAA) and Center for Colloid and Surface Science (CSGI), Università degli Studi del Molise, Via De
Sanctis, I-86100 Campobasso, Italy
b
Department of Medicine and Health Sciences “Vincenzo Tiberio”, Università degli Studi del Molise, Via De Sanctis, I-86100 Campobasso, Italy
c
Dipartimento di Bioscienze, Biotecnologie e Biofarmaceutica, Università degli Studi di Bari “Aldo Moro”, Bari, Italy
A R T I C L E I N F O
A B S T R A C T
Keywords:
Water treatment
TiO2
Photocatalysis
Dye
Kinetics
Fluorescence
Rhodamine B (RhB), a dye widely used in the textile manufacturing, contributes with other dyes to harm the
environment. Here, with the final goal to provide new tools for the removal of dyes from water, visible light
activated carbon-doped titanium dioxide was used to investigate on the decolourization and the photocatalytic
degradation of RhB dye from water solutions. The photodegradation activity was tested varying the initial
concentration of RhB and the amount of carbon-doped titanium dioxide, taking into account the ratio between
the amount of catalyst and the amount of RhB (TiO2/RhB), thus obtaining a parameter that allows the method to
be scaled up without losing its effectiveness. Values of k2 and t0.5 were obtained by fitting kinetics data to a
second-order kinetic adsorption model. The important role played by doped TiO2 particles is demonstrated by
the highly efficient color removal obtained during the visible light-induced photocatalysis. The presence of
different degradation intermediates was demonstrated by means of UV–vis Absorption and Fluorescence spectroscopy. Such results underline that the whole photodegradation process does not end with the decolourization
occurrence.
1. Introduction
Dye pollutants produced from the textile manufacturing are becoming a serious source of environmental contamination [1,2]. It is
estimated that thousands of different dyes and pigments are used industrially and an enormous number of synthetic dyes are yearly produced worldwide. Textile factories are second only to agriculture in the
amount of pollution they create and the large amounts of water they
use. Pollutants released by the global textile industry are continuously
doing incredible harm to the environment, polluting lands and making
them useless and unproductive [3].
Dyes are substances widely used in textile, as well as in pharmaceutical, food, plastics, paper manufacturing [4–8]. The chromophores,
responsible for the specific dye color, are classified according to their
chemical structure and their application field. The chromophore-containing centers are based on various functional groups, among these the
main are azo, anthraquinone, methine, nitro, arylmethane, carbonyl
groups. Donating substituents able to generate color amplification of
the chromophores are denominated auxochromes (amine, carboxyl,
sulfonate and hydroxyl).
Among these molecules Rhodamine B (RhB) is a fluorescent cationic
dye widely used in textile dyeing because of its more rigid structure
than other organic dyes, and is also a well-known fluorescent water
tracer [9]. Due to its cationic structure, it can be used for anionic fabrics
that contain negative charges such as polyester fibers. RhB results
harmful to human and animals: it causes irritation of the skin, eyes and
respiratory tract. Also, Rhodamine dyes are highly toxic to reproductive
and nervous systems and it has been proven that drinking water contaminated with Rhodamine could lead to subcutaneous tissue borne
sarcoma [10].
Worldwide regulations for industrial wastewater require significant
elimination of the dyestuff amount from the effluent [11]. Nevertheless,
it has been evaluated that a considerable part of the dyestuff is still
being released to the ecosystem. Several approaches have been developed for the effluent treatment but none of them is still sufficiently
effective and a combination approach seems to be so far the most
⁎
Corresponding authors at: Department of Agricultural, Environmental and Food Sciences and Center for Colloid and Surface Science (CSGI), Università degli Studi del Molise, via De
Sanctis, I-86100 Campobasso, Italy.
E-mail addresses: francesco.venditti@gmail.com (F. Venditti), lopez@unimol.it (F. Lopez).
1
These two authors contributed equally to this work.
http://dx.doi.org/10.1016/j.jwpe.2017.09.014
Received 18 August 2017; Received in revised form 7 September 2017; Accepted 18 September 2017
2214-7144/ © 2017 Elsevier Ltd. All rights reserved.
Journal of Water Process Engineering 20 (2017) 71–77
G. Cinelli et al.
efforts have been made to discover methods providing the photoactivation of this photocatalyst under visible light. Doping of TiO2 represents a widely used approach for developing TiO2 based materials
useful for environmental applications [18]. Different methods for the
synthesis of carbon doped TiO2 particles have been proposed to improve the photocatalytic activity [16,19]. Recently different research
groups highlighted the efficiency of a visible-light-active TiO2 photocatalyst prepared through carbon doping using glucose as the carbon
source towards organic compounds [20–22].
RhB is largely used to prove the efficiency of catalysts in general and
for TiO2 in particular, towards organic matter [23–27]. Nevertheless, as
stated above due to the possibility of incomplete degradation of the dye
molecule it would be useful to clarify the difference between decolourization and degradation. In fact, a decolourization process does not
necessarily correspond to a complete degradation of the dye [28].
Furthermore, the presence of different photocatalytic degradation
processes, such as chromophore cleavage, opening-ring, N-de-ethylation, and mineralization have also to be taken into account [29,30].
The aim of this investigation is the study of the photodegradation
process of the dye, RhB, induced by a carbon doped visible light-active
TiO2 photocatalyst. Furthermore, an accurate investigation of the decolourization and the photocatalytic activity of carbon doped TiO2 toward RhB was accomplished. The final goal is to provide new tools for
the challenging removal of dyes from water.
Fig. 1. Rhodamine B chemical structure.
efficient.
Generally, dyestuff is faced with chemical and physical methods,
such as adsorption and bio-treatment, co-precipitation, coagulation,
filtration, activated carbon, ozonation, and photochemical decolourization [12,13]. These methods frequently share the inconvenience of
incomplete degradation of the dye molecule, which leads to the formation of toxic by-products. These limits of conventional water treatment methods can be overcome by the use of advanced oxidation
processes, which have the ability to completely mineralize the dyes,
including the opening of the aryl ring. Usually, advanced oxidation
processes consist of procedures in which active hydroxyl radicals act as
strong oxidants for degradation of polluting materials. Most of these
processes are based on the high oxidation capacity of hydroxyl radicals
(2.8 V). One of the most effective methods among the advanced oxidation route is the use of UV rays combined with oxidant such as titanium dioxide.
Titanium dioxide (TiO2) is well recognized as a low cost and efficient catalyst for degradation of organic matters [14]. The application
of titanium dioxide as heterogeneous photocatalyst is well established
for the remediation of water and air purification [15,16]. For instance,
the photocatalytic degradation of azo dyes in aqueous solution is based
on photo activation of TiO2 with UV light, which leads to a sequence of
reactions resulting in the production of oxidants. The so formed compounds (hydroxyl radicals) can easily react with organic compounds on
the TiO2 surface [17]. However, since titanium dioxide has a band gap
of 3.2 eV, which can be activated only under UV-light irradiation,
2. Materials and methods
2.1. Materials
Glucose, titanium isopropoxide (97%), ethanol, potassium chloride,
sodium carbonate and Rhodamine B (RhB) were purchased from SigmaAldrich.
2.2. Carbon-doped titanium
Carbon-doped TiO2 (CDT) was synthesized following the method
reported by Ren et al. [21]. TiO2 particles were prepared by the hydrolysis of titanium isopropoxide in ethanol performed in the presence
of potassium chloride. The sample was continuously stirred to produce
Fig. 2. RhB UV–visible adsorption spectra and
sample decolourization pictures as a function of time
exposure to visible light irradiation. Inset λmax shift.
Ti/RhB: 150.
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G. Cinelli et al.
activated under visible light irradiation. Photocatalysis were performed
by placing the samples in a homemade reactor. The photocatalytic activity was activated with lamps providing visible light (6500 K). The
photoemission spectrum of the fluorescence lamps provides visible light
in the range of 400−800 nm. The distance between the light source and
the bottom of the solution was ∼15 cm. 10 mg of CDT were added to
10 mL of RhB solutions at different concentrations (6–60 mgL−1) and
mechanically stirred. The temperature was kept constant at 25 °C.
Samples were air-equilibrated and placed in the reactor and treated
with visible light. Aliquots of the sample were withdrawn, diluted 1:10
with water, centrifuged at 10000 rpm for 10 min and analyzed.
Changes in RhB concentrations due to water evaporation were taken
into account and corrected. Experiments were performed in duplicate,
and results were the mean values. The initial RhB concentration was
obtained by means of a calibration curve performed at 25 °C.
2.4. Spectroscopic characterization
The RhB decolourization was determined spectrophotometrically by
means of a double-beam thermostated spectrometer (Cary 100-Varian)
in the 200–800 nm region. The decolourization process was followed at
554 nm, and its extent was determined as the difference between initial
and final absorbance values and converted to concentrations values by
means of a calibration curve. The percentage of RhB decolourization
was calculated as normalized concentration (C/C0, where C0 is the initial concentration of RhB and C is the concentration of RhB at time t).
Fluorescence measurements were performed using a Varian Eclipse
spectrofluorimeter in a 1 cm quartz fluorescence cuvette, at 25 °C. The
excitation and the emission slit widths were 5 nm. The excitation wavelengths utilized for this study were 495, 510, 530 and 554 nm.
2.5. ζ potential
ζ potential measurements were performed by laser Doppler velocimetry using a Zetasizer-Nano ZS90 Malvern UK instrument operating
with a 4 mW He–Ne laser (633 nm wavelength).
2.6. Scanning electron microscopy (SEM)
Images were obtained with a Zeiss DSM 940 instrument. Samples
were deposited onto glass plates, left for 5 h at room temperature and
sputtered with gold.
Fig. 3. (A) RhB decolourization profiles as a function of time. RhB under light irradiation
with different amounts of carbon doped TiO2. TiO2/RhB ratios 20, 80 and 150. (B) Fitting
of the decolourization profiles to Eq. (1).
3. Results and discussion
Table 1
Values of k2, qe, and t0.5 at different TiO2/RhB ratio obtained by fitting the experimental
data to Eqs. (1) and (2).
TiO2/RhB
20
TiO2/RhB
80
TiO2/RhB
150
k2
(kg/g min)
qe
(g/kg)
t0.5
(min)
2.31 × 10−4 ( ± 1.32 × 10−5)
9.87 ( ± 0.46)
438 ( ± 32)
0.01 ( ± 0.002)
1.46 ( ± 0.11)
68 ( ± 12)
7.35 ( ± 0.93)
0.77 ( ± 0.03)
0.17( ± 0.022)
3.1. RhB decolourization
The photocatalytic activity of carbon-doped TiO2 (CDT) was tested
for the degradation of RhB (whose structure is reported in Fig. 1) by
lighting aqueous suspensions containing RhB and CDT particles with
visible light radiations.
CDT is made of a mesoporous material obtained by the substitution
of carbon atoms in the TiO2 with values of the band gap energy.
Micropore size and surface area are 3.01 eV, 8 nm and
126.5m2 g−1,respectively [21]. SEM images show that freshly prepared
CDT particles are monodisperse, in agreement with the method introduced by Ren and coworkers (see SI1) [21]. A significant aspect of
the whole photodegradation process is related to the surface charge of
CDT particles [22]. Value of ζ-potential in aqueous solution was
∼18 mV (data not shown).
First, the decolourization ability of carbon doped TiO2 towards RhB
at fixed appropriate amounts of CDT particles and RhB. Fig. 2 shows the
RhB adsorption spectra at different irradiation times was investigated.
At a first sight it can be easily appreciated that: i) the characteristic
absorption band of RhB at 554 nm rapidly decreases upon irradiation
and completely disappears in about 60 min; ii) a progressive
a white precipitate, and the obtained suspension was aged for 24 h. The
suspension after filtration was overdried to yield amorphous TiO2
particles. Carbon-doped TiO2 was synthesized by supplying a glucose
solution to amorphous TiO2 powder (0.25 g of TiO2 and 0.018 g of
glucose). The suspension was treated at 160 °C for 12 h and washed
several times with water and ethanol before use.
2.3. Rhodamine photodegradation
Photocatalytic degradation of RhB was carried out by using CDT
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Fig. 4. RhB fluorescence spectra at different excitation wavelengths as a function of visible light irradiation time. A:λex = 554 nm, B:λex = 530 nm; C:λex = 510 nm; D:λex = 495 nm.
Ti/RhB: 150.
Fig. 3A shows the decolourization ability of carbon doped titanium
for samples with different values of the ratio TiO2/RhB (20, 80 and 150)
during exposure to visible light irradiation. The experimental data,
expressed as normalized concentration (C/C0) of RhB as a function of
time at 25 °C, indicate that the RhB decolourization rate increases with
increasing TiO2/RhB ratios. The results are in agreement with a degradation process strictly related to the relative amounts of catalyst and
substrate, as well the ability of the substrate to be adsorbed on the
surface of the catalyst and other parameters, such as pH and O2 concentrations [22,31,32].
As shown, the kinetics becomes slower with time, reaching the
equilibrium after different time intervals depending on the TiO2/RhB
ratio. From the kinetics data, a dependence of the RhB decolourization
process on the TiO2/RhB ratio, typical of an adsorption process, was
demonstrated, foretelling a pivotal function of the adsorption event on
the photoreaction, in agreement with a recent study performed on
caffeic acid degradation in the presence of carbon doped TiO2 [22].
The decolourization profiles determined at different TiO2/RhB were
fitted to a second-order kinetics model by means of Eq. (1).
hypsochromic shift from 554 nm to 495 nm takes place. Fig. 2 also
reports the pictures of the sample during the photoreaction at different
time points. From a visual inspection of the sample it appears obvious
that the characteristic brilliant pink color of RhB rapidly disappears,
turning first into orange followed by yellow and white, in agreement
with the displayed spectra. Both blue shift and color variations suggest
the existence of different intermediates produced in the presence of
CDT under visible light irradiation. Such intermediates share an irradiation time dependent transient change of λmax starting from the initial RhB species at 554 nm (inset of Fig. 2). From these results, it is
evident that bleaching of the pink color (554 nm) does not correspond
to the whole RhB degradation process. The maximum absorption shift
from 554 to 495 nm with the increased illumination time has been
correlated in earlier studies performed in the presence of TiO2 and O2
with products coming from RhB N-de-ethylation [31].
The effect of the amount of substrate on the decolourization process
was next tested by focusing only on changes in absorbance at 554 nm.
Since from an applicative point of view it may be advantageous to
combine both TiO2 and RhB in a unique parameter, we elected to follow
the effect of different ratios between catalyst particles (mg of TiO2) and
amounts of dye (mg of RhB) [20].
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G. Cinelli et al.
Fig. 5. RhB emission wavelength shift according to the different excitation wavelength
(554, 530, 510 and 495 nm) as a function of irradiation time.
t
1
t
=
+
q
qe
k2 qe2
(1)
where k2 (kg/g per min) is the rate constant of a second-order adsorption, q and qe are the amounts of RhB adsorbed on CDT at time t
and at equilibrium, respectively (g/kg). The linear relationship, as reported in Fig. 3B, indicates that a second-order kinetics is applicable.
From Eq. (2) the half-life of the process can be calculated as:
t0.5 =
1
k2 qe
(2)
The k2, qe and t0.5 parameters at each TiO2/RhB ratio are presented
in Table 1. From these data, it emerges that the values of k2 increase
with the increase of TiO2/RhB ratio (thus, with the decrease of RhB
concentration) while, the qe values, as expected, decrease with increasing TiO2/RhB ratios. The t0.5 values represent suitable parameters
that underline the high decolourization rate attainable at high values of
TiO2/RhB ratios.
The low t0.5 value obtained with the TiO2/RhB 150 should not
surprise due to the large extent (excess) of the adsorption particles in
the earlier stages of the reaction [22].
3.2. RhB degradation
So far, we showed that CDT particles activated by visible light can
quickly decolorize RhB. Furthermore, as inferred from Fig. 2, the evidence of different peaks detectable during the photodegradation process suggests the presence of different photoprocesses. To further investigate this item we performed fluorescence measurements setting the
excitation wavelength in correspondence of some of the species identified through the adsorption maxima spectra (see Fig. 2), namely at
554 nm, 530 nm, 510 nm and 495 nm. Fluorescence spectroscopy has
been shown to be a valuable procedure to monitor wastewater as well
as an investigating tool on biological macromolecules [33–37]. Fig. 4
shows fluorescence spectra during the CDT mediated visible light RhB
degradation carried out at the specified excitation wavelengths. With
this approach the identification of at least 4 different intermediates is
ascertained. In fact, by focusing one by one on the different excitation
wavelengths, the presence and the evolution of transient species is well
deductible.
By exciting the RhB at 554 nm the only species that can be identified
is the one that emits at 574 nm. This species completely disappears
within 60 min of light exposure in the presence of CDT (Fig. 4A).
Fig. 6. RhB fluorescence spectra (at λex: 554,530,510,495 nm) at different times (0, 15,
45, 60, 105, 180, 300 min).
Exciting the Rhodamine at lower wavelengths revealed the existence of
other degradation intermediates. The excitation at 530 nm, indeed,
allowed the detection of a first N-de-ethylation product already after
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4. Conclusions
30 min of light exposure, corresponding to the blue shifted emission
maximum. Some species, however, were not well identified because
with the progress of the reaction other intermediates emitting at lower
wavelengths were produced. As apparent in Fig. 4B, the spectra collected starting from the 75 min time point cropped and are better
identified atλex = 510 nm until the 90 min time point. This inconvenience is overcome by exciting the sample at 495 nm. In this condition, after 105 min no more intermediates are formed and, during the
residual time, the degradation of the last intermediate occurs. Such
results underline that the whole photodegradation process does not end
with the decolourization occurrence.
Furthermore, by paying attention at the single emission peaks obtained with the different excitation wavelengths both the extent of intermediate lifetimes and the coexistence of intermediates can be identified as a function of the irradiation times (Fig. 5). The main
information of Fig. 5 other than the emission wavelength shift is the
fact that, after 15 min there are 3 or 4 different degradation intermediates of RhB. At least other 4 species are detectable at 30 and
45 min. After 1 h there are 3 species and after 105 min only one intermediate is detectable.
The time evolution of the fluorescence spectra at the different excitations lambdas confirms that all the photoprocesses are connected
(Fig. 6). In particular, by focusing on the black and the red spectra of
Fig. 6, referring to??ex of 554 and 495 nm, respectively, it is easy to
identify the two main species: the first reppresented by RhB that decomposes (λex 554 nm) and the last intermediate (λex 495 nm) that first
increases in intensity, than decomposes, decreasing in emission intensity. This evidence should be seen, therefore, as a very important
step forward in demonstrating that fluorescence spectroscopy is a suitable tool concerning the subject-matter addressed.
Our results, based on the presence of different intermediates during
RhB degradation in the presence of carbon-doped titanium dioxide are
in agreement with literature data [29,30,38]. In these studies the evidence of such intermediates were identified by HPLC and it was reported that intermediates were produced one by one and every intermediate was transformed from the one just before itself.
Moreover, the role of both the catalyst and the dye properties is well
established by the presence of two different photoprocesses, photobleaching and N-de-ethylation, that compete each other in the primary
steps of the photoreaction [31]. Specifically, it has been shown that the
formation of RhB+ is a prerequisite for photobleaching, while %OH is
responsible for the N-de-ethylation step. According to the oxidation
potential of RhB and the band edges of TiO2 the excited dye can inject
electrons into the conduction band of TiO2, particles which become
themselves cationic radicals and undergo further transformation to
products [39]. The photosensitization reaction possibly includes the
following reactions RhB + hν → RhB* + TiO2 → RhB+ + TiO2 (e).
Alternatively, in the presence of O2 upon visible light irradiation,
electrons can be excited directly into the TiO2 conduction band and
transferred to the adsorbed oxygen molecule to produce O2− and then %
OH with a strong oxidation power. Carbon doped titanium (CDT) used
in this study is characterized by the substitution of carbon atoms in the
TiO2 photocatalyst that adds new states close to the valence band edge
of TiO2 (band gap energy of 3.01 eV) [20,21]. Hereafter, the conduction
band edge shifts to narrow the band gap. The arrangement of carbon
into TiO2 leads to the formation of carbonaceous species, which promotes light absorption in the presence of visible light [18,32]. Meanwhile, the photogenerated hole oxidizes the adsorbed water molecule
(OH−) to produce %OH radical. The adsorbed dye can thus react with %
OH radical and be mineralized into CO2 and H2O after a series of reactions [40]. Accordingly, to perform the whole RhB degradation all the
criteria such as the presence of O2 and visible light have to be met.
Therefore, carbon doped titanium dioxide in the presence of visible
light fulfils the conditions to avoid eventual competitive reaction that
do not allow the whole RhB degradation process consisting in N-deethylation, chromophore cleavage, opening-ring, mineralization [29].
The present study, centered on the removal of Rhodamine B from
aqueous solutions, highlights the potential application of this technology for the elimination of dyes from wastewater, a fundamental goal
in both the environmental and agronomical fields. Rhodamine B was
degraded in the presence of carbon-doped TiO2 through a photocatalytic process activated by visible light. Kinetics data obtained by
means of UV–vis spectroscopy revealed high degradation rate and
substrate concentration dependence. The importance of adsorption
process and visible light for such kind of catalyst is confirmed [22].
Fluorescence Spectroscopy allowed understanding that the degradation
process of RhB was more than a simple adsorption based decolourization process, but passes through the formation of a series of intermediates generated from the N-de-ethylation reaction and gave information on the formation and co-existence of different intermediates.
Such kind of evidence is in agreement with previous studies [28,29].
Furthermore, the synergic presence of carbon-doped titanium dioxide
and visible light is an important condition to avoid the occurrence of
competitive reactions that could affect the whole RhB degradation
process [29].
Appendix A. Supplementary data
Supplementary data associated with this article can be found, in the
online version, at http://dx.doi.org/10.1016/j.jwpe.2017.09.014.
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