International Journal of Pure and Applied Mathematics Volume 119 No. 12 2018, 6345-6359 ISSN:1314-3395(on-lineversion) url:http://www.ijpam.eu SpecialIssue ijpam.eu SYNTHESIS AND CHARACTERIZATION OF BISMUTH OXIDE DOPED TITANIUM DIOXIDE AND ITS ANTIBACTERIAL ACTIVITY MAGESAN.P1, SVIARANJANI.A2, 1,2Associate Professor, Department of Chemistry, BIST, BIHER, Bharath University,Chennai-73 [email protected] Abstract Bi O -TiO nanocomposites were successfully synthesized by Sol-Gel method using 2 3 2 CTAB as templating agent. The synthesized materials were characterized by X-Ray Diffraction (XRD), Energy Dispersive X-ray (EDX) spectra, Scanning Electron Microscopy (SEM), Diffuse Reflectance Spectroscopy (DRS), Fourier Transform Infra-Red spectroscopy (FT-IR) and FT- Raman Spectroscopy (FT-Raman). Visible light photocatalytic activity of the samples was investigated by using Methyl orange dye. Furthermore, the antibacterial activity of the nanocomposites was tested against gram negative bacteria (Escherichia coli). Keywords: Composites, Sol-gel method, Semiconductivity, Antibacterial activity, spectroscopical studies. 1. Introduction In recent years, semiconductor photocatalysts have gained significant attention in the degradation of environmental contaminants[1-5]. Various semiconductor photocatalysts such as TiO [6], ZnO[7] and CdS [8] has been used for the environmental remediation process. Among the 2 various oxides semiconductor photocatalysts[6-11], TiO has been proven to be the most suitable 2 material due to its powerful oxidation strength, low cost, non-toxicity and chemical stability against photo corrosion and chemical corrosion[9-11]. In spite of the search for the idyllic 6345 International Journal of Pure and Applied Mathematics Special Issue photocatalyst for more than a couple of decades, titania (TiO ) in its anatase form, has persisted 2 as a touchstone photocatalyst against the activity of any emerging material is evaluated[12-21]: Typically, the conventional TiO photocatalyst would predictably meet an obstacle when applied 2 in practical applications such as effective utilization of UV/solar light, large surface area requirement for the adsorption of pollutant, that is, adverse recombination of electron and holes[22-29]. Efforts have been made to extend the adsorption of light from UV to visible region and to improve the photocatalytic efficiency of TiO [30-36]. Dopants like transition metals (Fe, 2 Al, Ni, Cr, Co, W, V and Zr) and metal oxides (Fe O , Cr O , CoO , SiO , etc.,) being used to 2 3 2 3 2 2 improve its applicability[13-15]. Reviews of Zeleska [16] has been discussed the method of preparation of doped TiO with metallic and non-metallic species; as well as different types of 2 dopants and doping materials. Doping of visible light active material on TiO nanopowders may 2 shift the absorption threshold of TiO from UV to visible region and the photocatalytic 2 efficiencies can be higher than the pure TiO and Degussa P25[17-20]. And also doping or 2 deposition of nobel metals on titania influence the photocatalytic activity by extending the excitation wavelength from ultraviolent region to visible region[37-42] Sol-gel synthesized SnO -TiO composite nanoparticles show larger photocatalytic activity to degrade rhodamine B 2 2 than TiO [29]. This is due to the extended optical response, improved charge separation, etc. Also, 2 the sol-gel synthesized SnO -TiO composite films exhibit higher surface hydroxyl group density 2 2 and photocatalytic activity than pure TiO under solar irradiation[30]. The photocatalytic 2 degradation of methylene blue by Sn-doped anatase TiO nanobelts, synthesized by a two-step 2 hydrothermal treatment, increases with Sn-content under visible-light illumination[31]. Sn-doped TiO or SnO -TiO composites have been obtained by sol-gel[32-34] or solvothermal[35] or 2 2 2 metalorganic decomposition[36] methods[43-45]. 6346 International Journal of Pure and Applied Mathematics Special Issue In this work, we have synthesized 4 % Bi O -TiO by simple precipitation method and their 2 3 2 spectroscopical studies were carried out. Methyl orange dye was used as a pollutant to determine the photocatalytic degradation of the prepared catalysts under solar light. Furthermore, the antibacterial activities of the nanocomposites were tested against gram negative bacteria (Escherichia coli) under dark condition. 2. Materials and methods 2.1. Materials Titanium Tetra IsoPropoxide (TTIP were purchased from Spectrochem, Tin Oxide (Bi O ) 2 3 from SRL, Methyl orange from S.D. Fine Chemicals and Isopropyl alcohol (IPA) from RFCl (RANKEM) were purchased and used as received. Freshly prepared de-ionized water was used in all the experiments. 2.2. Photocatalysts synthesis To synthesize TiO , Bi O -TiO nanoparticles, a sonochemical method was 2 2 3 2 applied. The approach for sonochemical synthesis of the above said nanocomposites was as follows: TTIP was dissolved in isopropyl alcohol at a volume ratio of 3:10, followed by the addition of an appropriate amount of metal oxide (Bi O ). The solution was sonicated for 1 hr in 2 3 bath type sonicator (EQUITRON) with frequency and a heating arrangement for the sonochemical synthesis of Bi O -TiO nanoparticles. The alkoxide solution after ultrasonic 2 3 2 mixing was added drop wise to 200 ml of 0.3 M Nitric acid aqueous solution in an ice/water bath under vigorous stirring to form a transparent homogeneous solution. Ammonia solution (0.3M) 6347 International Journal of Pure and Applied Mathematics Special Issue was added drop wise until the pH of the solution reached around 9. After aging for 12 hrs, the resulting white gel thus formed was separated by centrifugation and washed thoroughly by water followed by ethanol to remove the impurities. Finally, it was dried in an oven at 80 °C for 6 hr, followed by sintering at 500 °C for 3 hr. Instrumentation and Analysis The following physiochemical techniques have been used to characterize the prepared catalysts. To characterize the phase structure of the Bi O -TiO nanoparticles; a Bruker 2 3 2 D2 Phaser Desktop X-ray Diffractometer equipped with Ni-filtered Cu Kα radiation (λ=1.542 Å) and operated at an accelerating voltage and emission current of 30 kV and 10 mA, respectively. Data were acquired over the range of 2θ from 0° to 70 °C with a step size of 0.0017 and a scan rate of 7°/min. Scanning Electron Microscopy (SEM) was performed to examine the surface morphology of the prepared nanocomposites using DXS-10 ACKT scanning electron microscope equipped with EXS, which was used to study the elemental composition. Besides, the obtained SEM images were analyzed using manual microstructure distance measurement software to determine the diameter size distribution of the nanomaterials. Diffuse reflectance spectroscopy (DRS) spectra of the samples were recorded using Shimadzu 2100 UV-Visible spectrophotometer in the range of 200-800 nm equipped with an integrating sphere and BaSO 4 was used as the reference. For Fourier transform infrared spectroscopy (FT-IR) analysis, the KBr pellets were prepared from Bi O -TiO powders. FT-IR analysis was performed using a 2 3 2 spectrophotometer (Perkin Elmer RX1 instrument). Fourier transform Raman spectroscopy (FT- RAMAN) spectra of the prepared nanocomposites were recorded by using BRUKER RFS 27 spectrometer. Thermogravimetric-differential thermal analysis (TG-DTA) of the nanocomposites was taken on WATERS SDT Q 600 TA model instrument. 6348 International Journal of Pure and Applied Mathematics Special Issue Determination of Antimicrobial activity The antibacterial action of the prepared nanocomposites was examined using gram negative bacteria (Escherichia coli ATCC 25922) by well diffusion method. The prepared Nutrient agar was poured in the sterile Petri dishes and allowed to solidify. 24 h growing bacterial cultures (E. coli) were swabbed on it. The 5 wells (10 mm diameter) were made by using cork borer. The four different concentrations (250 µg, 500 µg, 750 µg and 1000 µg) of the nanoparticle, one negative control (tetracycline) were loaded in the wells. The plates were then incubated at 37 ºC for 24 hour. After incubation, the inhibition diameter was measured and the percentage of inhibition was calculated by using the formula (Eq. 1) I (Diameter of the Inhibited Zone) % of inhibition= -------------------------------------------- X100 (1) 90 (Diameter of the Petri-plate in mm) 3. Results and Discussion 3.1. XRD analysis of Bi O -TiO nanocomposites 2 3 2 XRD pattern of the prepared nanocomposites are given in the Fig.1. In all the synthesized nanocomposites, TiO exists in anatase phase show their sharp 2 characteristic peaks at 2θ= 24.8°, 37.3°, 47.3°, 53.4°, 54.3°, 62.2° and 68.5° corresponds to the (101), (004), (200), (105), (211), (204), (116), (220) and (215) planes agree well to standard JCPDS card No. 89-4921 and hence confirms that the nanocomposite have been predominantly 6349 International Journal of Pure and Applied Mathematics Special Issue crystalline in nature with anatase phase. The XRD patterns for Bi O -TiO show the peaks at 2 3 2 2θ=37.8°, 2θ=29.7° corresponding to Bi O (78-1793). The average crystallite sizes of the 2 3 nanocomposites have been deduced from the half-width of the full maximum (HWFM) of the 101anatase peak of TiO using Scherrer equation (Eq. 2), 2 t = K/cos, (2) Where t is the crystallite size, K is the shape factor of value 0.9, is the wavelength of the X-ray used. is the Bragg’s diffraction angle, is the corrected line broadening, = - , b s is the broadened profile width of the experimental sample and is the standard profile width b s of the reference (high purity silica) sample. According to the Eq. 2, the average crystallite sizes of the doped TiO nanocomposite are listed in the table 1 2 3.2. FT-IR analysis 6350 International Journal of Pure and Applied Mathematics Special Issue The FT-IR spectra of the undoped and doped TiO nanoparticles prepared by 2 sonochemical method are shown in the Fig.2. The results of FTIR analysis show four main absorption peaks located at 650-800, 1600-1700, 2360-2400 and 3450-3500 cm-1. The presence of strong transmittance band at 3400 cm-1 is attributed to the stretching vibrations of the O-H groups. A weak band at around 2300 cm-1 may be attributed to the vibrations of atmospheric CO 2 and the band appearing at 1630 cm-1 can be assigned to the angular deformation of water δH-OH. The appearance of band between 650 and 800 cm-1 are due to different vibrational modes of TiO . In addition to this rutile and anatase TiO phase absorption bands appear in the regions of 2 2 800-650 cm-1and 850-650 cm-1, respectively. Similar results have been matching with those reported in the literature. Scanning Electron Microscopy 6351 International Journal of Pure and Applied Mathematics Special Issue Fig. 5 shows the surface morphologies of the Bi O -TiO nanocomposites. As can be seen in 2 3 2 Fig. 5, the synthesized nanocomposites have non-uniform size, which may be a result of the aggregation of the doped TiO nanocomposites with spherical shape and the growth of irregular 2 crystalline grains during synthesis. According to the SEM images and using Manual Microstructure Distance Measurement software, the mean particle size of the doped TiO 2 nanocomposites were found and listed in the table 1. As can be seen, the diameter distribution of most of the particles in the range of 30-60 nm. Energy dispersive spectroscopy The composition is very sensitive for the application; therefore the elements present in the nanomaterials were scanned by EDS. The energy dispersive spectra of the prepared nanocomposites were recorded in the binding region of 0-10 keV which is shown in the Fig. 6. The signals and the atomic percentages from the spectrum reveal the presence of Ti, O, Bi, in the 6352 International Journal of Pure and Applied Mathematics Special Issue prepared nanocomposites. Though the peaks of Bi are insignificant in the Bi O -TiO 2 3 2 nanocomposites owing to its content in TiO matrix, the atomic percentages indicate the Bi 2 particles present in the nanocomposite. There is no trace of any other impurities could be seen within the detection limit of energy dispersive spectrum. (b) FT-Raman Spectroscopy Raman spectroscopy is a technique which is flexible and availed for studying the different phases of matter. Raman scattering spectra of Bi O -TiO nanocomposites were 2 3 2 recognized and displayed in the Fig.7. The frequencies of the raman bands observed for anatase TiO (in the powder doped with 2 Bi O ,) is at 140-150, 390-400, 510-530, 620-650 cm-1 are shown in the Fig.7. According to( bth) e 2 3 reported literature raman bands for anatase TiO are at 146, 198, 320, 398-448, 515, 640 and 796 2 cm-1[65]. As noted above, the band at about 146 cm-1 is the strongest of all the observed bands. Group theory depicts six raman active modes for the tetragonal anatase phase: three E modes g centered around145, 197 and 639 cm-1; two B modes at 399 and 519 cm-1; and one A mode at 1g 1g 513 cm-1[66]. From these results the bands at 198 cm-1 and 640 cm-1 are attributed to the E modes g and the one band at 400 cm-1 to the B modes and a doublet band at 520 cm-1 is assigned to A 1g 1g and B modes. These observances are comparable with the reported literature 1g 6353 International Journal of Pure and Applied Mathematics Special Issue Antimicrobial activity The antibacterial activity of the Bi O -TiO and TiO nanocomposites was investigated 2 3 2 2 by adopting well diffusion method against E. coli bacterial strains under dark condition. The zone of inhibition of the synthesized nanocomposites against E. coli is represented in the table 2. From the results of zone of inhibition method, it is observed that the Bi O -TiO shows 2 3 2 significant inhibition around the films (Fig.10). TiO nanocomposites under dark condition. 2 6354
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