Article

Efficient visible light active Polyaniline/TiO2 nanocomposite photocatalyst for degradation of Reactive Blue 4

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Abstract

Visible light active photocatalysts are much sought after due to possibility of development of efficient and less expensive photoreactors for environmental applications. We prepared a visible light active photocatalyst, situ polymerisation method. It was characterized using polyaniline-TiO2 photocatalytic activity of the PANI-TiO2 was tested for photo degradation of Reactive Blue 4 (RB-4) using visible (100 W tungsten-halogen lamp) as well as UV lamp (125 W). The PANI/TiO2 having thin layers of PANI (~1 nm) polymerized on the surface of TiO2 The nanocomposite displayed remarkable photocatalytic activity under visible light irradiation (% RB-4 removal efficiency ≥ 92; % TOC removal ≥ 50). About 15 times greater rate constant for the reaction under visible light (5.23 × 10-2 min-1) was obtained compared to the rate constant with TiO2 morphological data were discussed in the light of the reported data for PANI/TiO2 by different methods. On the basis of such comparison, a in which TiO2 PANI/TiO2 polyaniline could be inferred to have higher photo activity over the other forms. (PANI-TiO2 nanoparticles (~30 nm) were obtained. (k = 3.5 × 10-3 min-1). The kinetic and materials produced earlier nanoparticles are deposited on polyaniline could be inferred to have higher photo activity over the other forms.

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... However, after generated abundant amounts of protons and electrons by photocatalytic activity, the produced amount of CH4 and CO was reversed because the generation of CH4 is thermodynamically easier than that of CO as expressed in equation (3) and (4) [1]. In this study, the polyaniline coated onto the PBNO surface much enhanced CO2 conversion efficiency because it can behave as an electron conductor under the visible light irradiation [8]. As shown in Fig. 4, the PBNO/10%CP/GF exhibited the highest CO2 conversion efficiency and the production rates of CH4 and CO were 72.76 and 54.36 (μmol g -1 cat. ...
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... E. Subramanian et al., reported the photodegradation of MB dye using PANI-TiO 2 nanocomposite (Subramanian et al., 2014). S. Masid et al. reported the degradation efficiency of PANI-TiO 2 nanocomposite for reactive blue 4 (RB-4) (Masid et al., 2015). ...
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... 39 The authors suggested that PANI played an active role in the degradation of p-cresol by TiO 2 /ZnO/PANI by transferring electrons to the conduction band of TiO 2 /ZnO and also trapped holes, leading to charge separation. 39 In another study, Masid et al. suggested the same mechanism when they used PANI/TiO 2 to degrade a dye, reactive blue 4. 79 However, there is no experimental data to support the suggested degradation mechanisms. In this study, we provide experimental data showing which reactive oxygen species were responsible for the degradation. ...
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... The RuO2-TiO2/DPA/PANI nanocomposite has the same optical properties as the PANI; the corresponding spectrum is almost similar to that of the polyaniline represented in the literature [61,62]. The spectrum reveals the increase of the absorbance with the appearance of a small wave between 469 and 510 nm, corresponding to the π-π* transition in the polymeric chain [63]. The increase in the absorption of the two nanocomposites is due to the delocalization of the carrier's n-π* [64]. ...
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AbstractA PANI/TiO2 composite film deposited on the glass surface was successfully prepared using sol-gel dip-coating technique and chemical oxidation method. The film was characterized using XRD, AFM, and UV. The result showed that the TiO2 film consists of both cuboid-shaped and anatase-phased TiO2 nanoparticles. The average grain size of TiO2 in the film was approximately 20 nm. After coating with PANI, the particle was changed into irregular spherical-shaped and the size was increased up to approximately 35 nm in diameter. UV-Vis spectroscopy analysis indicated that the coating of TiO2 with PANI would result in an enhancement of photocatalytic efficiency and an extension of the photoresponse of TiO2. The band gap of the PANI/TiO2 film was 3.18 eV. The photocatalytic property of the film was evaluated by the degradation of rhodamine-B. It was found that 67.1% and 83.2% of rhodamine-B could be degraded under sunlight and UV irradiation within 120 min using the PANI/TiO2 composite film as photocatalyst.
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Polyaniline (PAn) sensitized nanocrystalline TiO2 composite photocatalyst (PAn/TiO2) with high activity and easy separation was facilely prepared by in situ chemical oxidation of aniline from the surfaces of the TiO2 nanoparticles. The morphology, structure, and light absorption properties of composite photocatalyst were examined in term of its application to photocatalysis. The photocatalytic activity of PAn/TiO2 nanocomposites for the degradation of methylene blue (MB) aqueous solution was investigated and compared with pure TiO2. The spectra analyses illustrated that, when PAn deposited on the surface of TiO2, the crystalline behavior of PAn was hampered and the degree of crystallinity decreased, and the characteristic peaks of the PAn were shifted indicating that there was a strong interaction between PAn and TiO2 nanoparticles. PAn was able to sensitize TiO2 efficiently and the composite photocatalyst could be activated by absorbing both the ultraviolet and visible light (λ = 190–800 nm), whereas pure TiO2 absorbed ultraviolet light only (λ
Article
This study investigated the role of the band gap, surface area, and phase composition on the photocatalytic activity of nanocrystalline TiO2. Nanocrystalline TiO2 (8-29 nm) was synthesized by hydrolysis of titanium tetraisopropoxide. The crystalline structure, band gap, and morphology of the nanocrystalline TiO2 were determined by X-ray diffraction (XRD), diffuse reflectance spectroscopy (DRS), and N-2 adsorption (BET) at 77 K, respectively. It is observed that the band gap of the nanocrystalline TiO2 decreases from 3.29 to 3.01 eV with increasing calcination temperature. The crystallite size of the TiO2 samples prepared also shows an increase with increasing calcination temperature. The photocatalytic degradation of an aqueous solution of nitrobenzene (50 ppm) was studied using nanocrystalline TiO2 samples with varying band-gap values, as well as a P-25 Degussa TiO2 sample for comparison. The initial rate of degradation of nitrobenzene was calculated in each case to evaluate the photocatalytic activity of the catalysts. The enhanced photocatalytic degradation of nitrobenzene was observed by purging air through the solution during photocatalysis.
Article
Polythiophene/titanium dioxide (PT/TiO2) composites were prepared by the in situ chemical oxidative polymerization method. The resulting PT/TiO2 composites were characterized by Fourier transform infrared (FT-IR) spectroscopy, ultraviolet–visible (UV–Vis) diffuse reflectance spectroscopy, X-ray photoelectron spectroscopy (XPS), X-ray diffraction (XRD) and field emission scanning electron microscopy (SEM). UV–Vis diffuse reflectance spectra measurements show that the PT/TiO2 composites can adsorb light of wavelengths ranging from 200nm to 800nm. The PT/TiO2 composites showed good adsorption properties and were more efficient in removing dye from solution than pure PT and pure TiO2. The PT/TiO2 composites exhibited photocatalytic activities to some extent under UV light illumination.
Article
Polypyrrole/TiO2 composite is prepared by in situ polymerization of pyrrole on the TiO2 template. The TiO2 microbelts are prepared by sol–gel method using the absorbent cotton template for the first time. Then the TiO2 microbelts are used as template for the preparation of polypyrrole/TiO2 composites. The structure, morphology and properties of the composites are characterized with scanning electron microscope (SEM), IR and Network Analyzer. A possible formation mechanism of TiO2 microbelts and polypyrrole/TiO2 composites has been proposed. The effect of the molar ratio of pyrrole/TiO2 on the photocatalysis properties and microwave loss properties of the composites is investigated.
Article
PANI modified core–shell mesoporous TiO2 (PANI/M-TiO2) with efficient photocatalytic capability under visible light irradiation was fabricated by hydrothermal method and chemisorption approach. The nitrogen adsorption–desorption characterization indicated that the specific surface area of mesoporous M-TiO2 was 2.8 times as great as that of P25, which resulted in the increased uptake of PANI molecule on the surface of M-TiO2. Environmental scanning electron microscopy and transmission electron microscopy images demonstrated that the PANI/M-TiO2 possessed a unique core–shell structure, which allowed multiple reflection or scattering of light in the photocatalyst and led to the increase of optical path length subsequently. Both the increased uptake of PANI molecules and optical path length in photocatalyst contributed to enhance the visible light absorption. The UV–vis diffuse reflectance spectra confirmed that the optical absorption for PANI/M-TiO2 was more intensive than that for PANI modified TiO2 nanoparticle (PANI/NP-TiO2) in the visible light region. The intensive visible light absorption and effective charge separation owing to the heterojunction built between TiO2 and PANI lead to remarkable improvement of visible light photocatalysis. The pseudo-first-order kinetic constant of photocatalytic degradation of rhodamine B and 4-chlorophenol under visible light irradiation with 6% PANI/M-TiO2 was 5.04 and 2.03 times as great as that with PANI/NP-TiO2 respectively, showing the advantage of the unique core–shell mesoporous structure in the PANI/M-TiO2 for efficient photocatalysis.
Article
Titanium dioxide doped polyaniline has been prepared by in situ polymerization. TiO2 nanoparticles with an average diameter about 20 nm were used as a dopant of polyaniline. The doping effect of TiO2 was characterized and evaluated by scanning electron microscopy (SEM), Fourier transformation infrared spectroscopy (FT-IR), energy dispersive spectrometry (EDS) and electrical conductivity measurement. SEM study shows that TiO2 nanoparticles have a strong effect on the morphology of composites. The FT-IR spectra reveal that the interaction between TiO2 and polyaniline (PANI) is primarily based on the formation of H-bonding. Electrical conductivity measurements indicate that the conductivity of composites at low TiO2 content is much higher than that of neat PANI, while with the increasing contents of TiO2, the conductivity shows an orderly decrease.
Article
Nanosized C-doped TiO 2 was prepared by a new method based on resorcinol-formaldehyde (RF) gel formation in situ during hydrolysis of Ti precursor (TTIP, titanium tetraisopropoxide). XRD, DRS, EDX, SEM and HRTEM results confirmed that the carbon in the sample existed as free carbon (C–C), carbonate carbon (–CO 3 ) and doped into lattice of TiO 2 (Ti–C), resulting in red shift of optical adsorption edge and band gap narrowing. The photo activity of the C-doped TiO 2 , tested on 2-chlorophenol, revealed that it was more active under visible light (k vis = 3.50 × 10 −3 min −1 ).
Article
This paper describes the photoelectrochemical response in aqueous electrolyte of nitrogen-doped titanium dioxide, TiO2-xNx. Thin film electrodes were prepared by reactive DC magnetron sputtering in an environment of Ar, O2, and N2. A typical film thickness was 0.85 μm. The crystal structure of the photoelectrochemically active films was mainly of rutile character, and scanning and transmission electron microscopy showed a highly porous parallel penniform nanostructure. It was conclusively shown that dioxygen could be generated from water by illumination of the TiO2-xNx electrodes at moderate anodic potentials. The current density under 1000 W m-2 visible light from a sulfur lamp was 0.2 mA cm-2 at 0.55 V vs Ag/AgCl. Current−voltage characteristics under illumination were strongly dependent on the scan direction. Scanning the electrode from cathodic toward anodic potentials gave an onset potential similar to that of normal rutile TiO2, whereas a reversed scan gave an onset of photocurrent (depending on the light source) anodically upshifted by up to 0.8 V from its normal position. Moreover, a cathodic current was observed during the latter scans. This current was induced by the illumination at anodic potentials. This nonfaradic current was ascribed to photoinduced electron trap states distributed in an approximately 1.3 V wide range negative of the conduction band (CB) edge. These states also were active as electron−hole recombination centers. The density of this new set of states was 2 × 1020 cm-3, i.e., similar to the density of nitrogen atoms. They can be activated by light, even at wavelengths beyond 700 nm, and work as long-lived electron traps; hence, they have properties that are different from those of the earlier found Ti3+ (3d) states, also located below the CB of TiO2. The new states occur as a consequence of the nitrogen doping, but is not necessarily an intrinsic property of pure TiO2-xNx. Recombination via the new statesin conjunction with slow hole transport in the nitrogen-created band above the valence band edgewas suggested to be the cause of the large anodic shift of the onset potential for cathodic scans and of the moderate water oxidation efficiency of the TiO2-xNx thin film electrodes.
Article
A systematic study of metal ion doping in quantum (Q)-sized (2-4 nm) TiO_2 colloids is performed by measuring their photoreactivities and the transient charge carrier recombination dynamics. The presence of metal ion dopants in the TiO_2 crystalline matrix significantly influences photoreactivity, charge carrier recombination rates, and interfacial electron-transfer rates. The photoreactivities of 21 metal ion-doped colloids are quantified in terms of both the conduction band electron reduction of an electron acceptor (CCl_4 dechlorination) and the valence band hole oxidation of an electron donor (CHCl_3 degradation). Doping with Fe^(3+), Mo^(5+), Ru^(3+), Os^(3+), Re^(5+), V^(4+), and Rh^(3+) at 0.1-0.5 at.% significantly increases the photoreactivity for both oxidation and reduction while Co^(3+) and Al^(3+) doping decreases the photoreactivity. The transient absorption signals upon laser flash photolysis (λ_(ex) = 355 nm) at λ = 600 nm are extended up to 50 ms for Fe^(3+)-, V^(4+)-, Mo^(5+)-, and Ru^(3+)-doped TiO_2 while the undoped Q-sized TiO_2 shows a complete "blue electron" signal decay within 200 μs. Co^(3+)- and Al^(3+)-doped TiO_2 are characterized by rapid signal decays with a complete loss of absorption signals within 5 μs. The quantum yields obtained during CW photolyses are quantitatively correlated with the measured transient absorption signals of the charge carriers. Photoreactivities are shown to increase with the relative concentration of trapped charge carriers. The photoreactivity of doped TiO_2 appears to be a complex function of the dopant concentration, the energy level of dopants within the TiO_2 lattice, their d electronic configuration, the distribution of dopants, the electron donor concentration, and the light intensity.
Article
Titanium dioxide nanoparticles were modified by polyaniline (PANI) using ‘in situ’ chemical oxidative polymerization method in hydrochloric acid solutions. Powder X-ray diffraction (XRD), transmission electron microscopy (TEM), Fourier-transform infrared spectra (FT-IR), X-ray photoelectron spectroscopy spectrum (XPS) and UV–vis spectra were carried out to characterize the composites with different PANI contents. The photocatalytic degradation of phenol was chosen as a model reaction to evaluate the photocatalytic activities of the modified catalysts. Results show that TiO2 nanoparticles are deposited by PANI to mitigate TiO2 particles agglomeration. The modification does not alter the crystalline structure of the TiO2 nanoparticles according to the X-ray diffraction patterns. UV–vis spectra reveal that PANI-modified TiO2 composites show stronger absorption than neat TiO2 under the whole range of visible light. The resulting PANI-modified TiO2 composites exhibit significantly higher photocatalytic activity than that of neat TiO2 on degradation of phenol aqueous solution under visible light irradiation (λ ≥ 400 nm). An optimum of the synergetic effect is found for an initial molar ratio of aniline to TiO2 equal to 1/100.
Article
TiO 2 (110) single crystals, doped with nitrogen via an NH 3 treatment at 870 K, have been found to exhibit photoactivity at photon energies down to 2.4 eV, which is 0.6 eV below the band-gap energy for rutile TiO 2 . The active dopant state of the interstitial nitrogen that is responsible for this effect exhibits an N (1s) binding energy of 399.6 eV and is due to a form of nitrogen that is probably bound to hydrogen, which differs from the substitutional nitride state with an N (1s) binding energy of 396.7 eV. Optical absorption measurements also show enhanced absorption down to 2.4 eV for the NH 3 -treated TiO 2 (110). A co-doping effect between nitrogen and hydrogen is postulated to be responsible for the enhanced photoactivity of nitrogen-doped TiO 2 materials in the range of visible light.
Article
The photoreactivity of sol-gel (SG)-TiO2 films was enhanced significantly with addition of a small amount of trifluoroacetic acid (TFA) into the starting solution. The promoting effect was confirmed in two separate experiments of the methylsiloxane monolayer oxidation and the photocurrent measurements. The results of film characterization indicated that the absorption coefficient for ultraviolet light ( < 360="" nm)="" increases="" due="" to="" film="" densification="" and="" the="" crystallinity="" is="" improved="" upon="" f="" doping.="" the="" improvement="" in="" the="" photoreactivity="" was="" ultimately="" attributed="" to="" the="" increase="" in="" the="" rate="" at="" which="" the="" photogenerated="" charge="" carriers="" reach="" the="" surface="" in="" the="" photostationary="">
Article
A series of polyaniline (PANI)-sensitized TiO2 composite photocatalysts (PANI/TiO2) with different mass ratio of polyaniline to nano- TiO2 (P25) (1:200–1:700) were facilely prepared by mixing a tetrahydrofuran (THF) solution of camphorsulfonic acid (CSA)-doped polyaniline (PANI-CSA) and TiO2 nanoparticle suspension in ethanol. Transmission electron microscopy, X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS) and ultraviolet–visible diffuse reflectance spectroscopy (DRS) measurements were used to characterize the resulting composite photocatalysts, and their photocatalytic activities were investigated by degrading methylene blue (MB) under visible-light irradiation (). The results showed that the surface polyaniline sensitization had no effect on the crystalline structure but aggravated the agglomeration of TiO2 nanoparticles by forming multi-particles. After being sensitized by PANI, the light response of TiO2 was extended to visible-light regions and the photocatalytic activity of the composite photocatalysts was enhanced. MB could be degraded more efficiently on PANI/TiO2 than on the bare TiO2 when the mass ratio of polyaniline to TiO2 was in the range 1:400–1:700, and the optimum sensitized effect was found at a mass ratio of 1:500. The determined rate constant of MB degradation over PANI/TiO2 (1:500) was 0.01515 min−1, which is 1.57 times higher than that of bare TiO2 (0.00963 min−1). Furthermore, PANI/TiO2 composite photocatalysts showed good photocatalytic stability after five runs under visible light. The enhancement of photocatalytic activity of the composite photocatalysts could be attributed to the sensitizing effect of PANI. A possible mechanism for the photocatalytic degradation of methylene blue is also proposed.
Article
Scientific studies on photocatalysis started about two and a half decades ago. Titanium dioxide (TiO2), which is one of the most basic materials in our daily life, has emerged as an excellent photocatalyst material for environmental purification. In this review, current progress in the area of TiO2 photocatalysis, mainly photocatalytic air purification, sterilization and cancer therapy are discussed together with some fundamental aspects. A novel photoinduced superhydrophilic phenomenon involving TiO2 and its applications are presented.
Article
This paper presents the review of the effects of operating parameters on the photocatalytic degradation of textile dyes using TiO2-based photocatalysts. It further examines various methods used in the preparations of the considered photocatalysts. The findings revealed that various parameters, such as the initial pH of the solution to be degraded, oxidizing agents, temperature at which the catalysts must be calcined, dopant(s) content and catalyst loading exert their individual influence on the photocatalytic degradation of any dye in wastewaters. It was also found out that sol-gel method is widely used in the production of TiO2-based photocatalysts because of the advantage derived from its ability to synthesize nanosized crystallized powder of the photocatalysts of high purity at relatively low temperature.
Article
The kinetics of photocatalytic (TiO(2)/UV) degradation of 2-chlorophenol (2-CP), characterization of intermediates and induction of biodegradability in treated chlorophenol solutions is reported. Approximately 95% of the 2-CP is removed in approximately 2h at pH 5 and 0.2g TiO(2)l(-1) when the 2-CP concentration is < or =100mgl(-1); the pseudo-first-order rate constant (k) is estimated to be 0.0183 min(-1). GC-MS analyses detected phenol, catechol, hydroxyhydroquinone (HHQ), and chlorohydroquinone (CHQ) intermediates during the short irradiation time (<1h); however two other higher carbon intermediates 2-hydroxy-benzaldehyde (HB) and [1.1'-biphenyl]-2,2'-diol (BPD) are found as major intermediates over longer irradiation times. The biochemical oxygen demand (BOD) of treated 2-CP solutions improved substantially. A tentative mechanistic pathway to explain formation of higher carbon intermediates is presented.
Article
The dramatic visible light photocatalytic activity was obtained for the degradation of Methylene Blue (MB) and Rhodamine B (RhB) under visible light irradiation (lambda > 450 nm) after TiO2 photocatalysts were modified with monolayer dispersed polyaniline (PANI) via a facile chemisorption approach. Under visible light irradiation, PANI generated pi-pi* transition, delivering the excited electrons into the conduction band of TiO2, and then the electrons transferred to an adsorbed electron acceptor to yield oxygenous radicals to degrade pollutants. Also, the ultraviolet photocatalytic performance was enhanced to about two times compared with that of P-25 TiO2 photocatalyst. The high photocatalytic activity came from the synergetic effect between PANI and TiO2, which promoted the migration efficiency of photogenerated carriers on the interface of PANI and TiO2. Under ultraviolet light irradiation, photoinduced holes in TiO2 valence band could transfer into HOMO orbital of PANI and then emigrate to the photocatalyst surface and oxidize the adsorbed contaminants directly. The optimum synergetic effect was found at a weight ratio of 3.0 wt % (PANI/ TiO2).
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