Nowadays renewable energy sources are highly explored and preferred by a lot of developing and developed countries in order to minimize the greenhouse gas discharges.[1,2]. Ferrites are iron-containing compounds that are categorized into spinels, hexagonal ferrites and garnets . Nano-structured iron containing transition metal oxide materials are known to exhibit interesting physical and chemical properties. In addition, these properties are significantly different from those of conventional bulk materials owing to their extremely small size and large surface area. Ferrites of the form MFe2O4 (M = Ni2+, Co2+, Cu2+, Zn2+, etc.,) have been gaining considerable momentum as they are highly used in the electronic materials industries. Other transition metal oxides that have been widely investigated are oxides of copper, cobalt and nickel . Fd3m is the space group for the structure of spinel ferrite. The cubic unit cell consists of 56 atoms, 32 oxygen anions which are distributed in a cubic close-packed structure. Here, 24 cations occupy 8 of the 64 available tetrahedral sites (A sites) and 16 of the 32 available octahedral sites (B sites) . The distribution of cation depends on the electronic configuration and valence of ions. The useful properties of ferrite nanoparticles depend on both sizes as well as cation distribution. If the atom size decreases, the surface region increases. It results in improving the catalytic properties [6, 7]. Nevertheless, each nanoparticle can behave as a single magnetic domain. From the literature survey, it was found that changes in the particle size can determine the magnetic properties due to the change in cation distribution . Nanoparticle synthesis of these could be various methods such as sol-gel , sol-gel auto-combustion method , and co-precipitation method . Moreover, important properties of ferrites are determined by the cation site occupations at the tetrahedral and octahedral sub lattices [12, 13].
In the present work, Aim to study the prepared Zinc copper ferrite nanoparticles by chemical co-precipitation technique. The Characterization of the Structural, morphological and magnetic properties of the Zinc copper ferrite nanoparticles was analysed through powder XRD, TEM and VSM. Furthermore, the Photocatalysis property was also analysed.
MATERIALS AND METHODS
All the chemicals were analytical graded and used without further refining. Typically, the solution of 0.2M Fe (NO3) 3.9H2O, 0.08M Zn (NO3) 2.6H2O, 0.02M Cu (NO3) 2.6H2O and 0.5 g Polyethylene glycol 200 (PEG) were dissolved in distilled water with a constant stirring. The precipitating reagent ammonia hydroxide (25%) was added drop-wise into metal solutions, contained in a beaker, with constant stirring until co-precipitation occurred and the PH reached 10. The reaction temperature was maintained at 85 °C for 45 minute. The final product was dried in an oven at a temperature of 110 °C for 24 hrs to remove water contents and annealing at various temperatures such as 500 and 600⁰C for 2hrs was carried out.
The confirmation of spinel phase purity was evaluated by Powder XRD measurement. Morphological features were evaluated by SEM. Morphology, as well as the particle size of the sample, was probed using HRTEM. The photo-degradation experiments for methylene blue (MB) dye molecule over Zinc Copper ferrite, annealed at 600⁰C, were determined by measuring the absorbance value at approximately 484nm using a Shimadzu UV-2501PC spectrometer. Infrared spectra were obtained using Fourier transform infrared spectroscopy (FT-IR, Nicolet 6700) in the 400 - 4000 cm−1 range. The magnetic properties of these samples were carried out by Vibrating Sample Magnetometer (VSM) (model Lake Shore 7307) with an applied magnetic field range ± 10 KOe at room temperature.
RESULTS AND DISCUSSION
The crystalline structure of the Zinc copper ferrite as prepared and annealed at 500°C and 600°C are shown in Fig.1. All of the diffraction peaks can be indexed to the standard Zinc copper ferrite with the cubic spinel structure and the reflection peaks match well with standard data (JCPDS 82-1042). This indicates the synthesized nanoparticles have Fd3m space group and indicating high degree purity. The average crystallite sizes, D, are calculated from the (311) peaks through the Scherrer’s formula around 32 nm. It is observed that the sample Zn1-x CuxFe2O4 crystallized in cubic structure and the lattice parameter is found to be 8.355 Å, which is less than the values reported for bulk compounds. This is mainly because of the replacement of smaller Cu2+ ions (0.72 Å) by larger Zn2+ ions (0.74 Å) [14,15]. In addition, as the ionic radius of Zn2+ is larger than the ionic radius of Cu2+, the Zn2+ substitution leads to larger expansion of the lattice. Consequently, the lattice parameter increases more when compared to the Cu2+ substitution in the synthesized particles. Since ionic radius of Fe2+ (0.74 Å) ion is larger than Fe3+ ion (0.64 Å), the lattice constant increases . Nonmagnetic transition metal ions Zn2+ and Cu2+ ion prefer octahedral sites whereas Fe3+ ions prefer both tetrahedral and octahedral sites.
Scanning Electron Microscopy (SEM) and Energy dispersive X-Ray spectra (EDX) Analysis
Using the typical SEM analysis, morphological characteristics of Zinc copper ferrite nanoparticles annealed at 600°C are shown in Fig.2 (a). They show the formation of multigrain agglomerations consisting of fine crystallites with irregular shapes and sizes. Ferrite powders possessed a coarse structure with crystalline microstructure with an average grain size homogeneous is about 50 μm obtained from SEM images. This is larger than size of nanocrystals calculated using the XRD measurements, which, in turn, simply indicates that each grain is formed by aggregation of a larger number of nanocrystals. The samples are irregular shapes and sizes, and cohesion of grains is due to the magnetic attraction. A drastic difference in microstructure of the annealed at 600°C products indicated that the substitution to the metal ions like Zn, and Cu surface of these microstructure. EDX analysis confirms the stoichiometric proportion of Zinc copper ferrite nanoparticles annealed at 600°C and also the percentage proportion of the constituent elements is shown in Fig.2 (b). The elemental weight proportion percentage is presented in the tables of weight and atomic percentage proportions, the constituent elemental proportion and the ratios are in line with expected elemental proportion and the oxygen (O) and iron (Fe) being with highest peaks in all of the samples . Typical EDX analysis reveals the existence of elements of Zn, Cu, Fe, and O.
High Resolution Transmission Electron Microscopy Analysis (HRTEM)
As portrayed in Fig.3 (a), HRTEM micrographs also confirm the particle size of Zinc copper ferrite nanoparticles annealed at 600°C. The average crystallite size is around 8.38 nm. HRTEM analysis reveals that the particles are nearly spherical in shape. The average crystallite size estimated from HRTEM image is found to be in good agreement with the observed values from powder XRD results. From Fig.3 (b), HRTEM image of individual Zinc copper ferrite nanocrystal indicates that the interplanar distance is 0.26. In the SAED (Fig.3(c).) image of annealed at 600°C Zinc copper ferrite nanoparticles, the diffraction rings match well with standards powder XRD diffraction data that confirms good crystallinity. The observed crystallographic d values of 2.52 Å correspond to the lattice space of (311) plane of the Zinc copper ferrite system. The observed crystallographic d values agree well with those obtained from powder XRD analysis.
Fourier transform infrared spectroscopy (FT-IR) Studies
FT-IR spectra are usually assigned to the vibration of ions in the crystal lattice, which can be used to confirm the positions of Zn2+, Cu2+, and Fe3+ ions in spinel structure. The vibrating sample magnetometer is used to measure the magnetic properties of samples.
Fig. 4 shows the typical FT-IR spectra of Zinc copper ferrite nanoparticles recorded between 4000 and 400 cm−1. In the range of 1000 - 400 cm−1, The two main absorption bands at 522 and 862 cm−1 correspond to the Fe-O bonds in the tetrahedral and octahedral sites, respectively, confirming the spinel structure of Fe3O4 nanoparticles. Similar results are observed in Zinc copper ferrite nanoparticles prepared by sol-gel combustion method [18-21]. When Zn2+ ions are replaced by Cu2+ ions, due to charge imbalance some Fe3+ ions shift from A sites to B sites, making the Fe3+-O2 stretching vibration in greater. So the decrease in peak intensity of υ1 with increasing Cu2+ content is mainly attributed to the change in Fe3+-O2 bands. The broad peaks that appear from 3205 to 2978 cm−1 and the IR absorption peaks between 1350 and 1066 cm−1 are due to the fundamental and overtones O-H stretching vibrations of the hydroxyl groups of water on the nanoparticles, respectively . These results are consistent with the previous reports [23, 24]
Fig. 5 shows a typical hysteresis loop of all the Zinc copper ferrite nanoparticles compositions which are annealed at 600˚C. By using a vibrating sample magnetometer, the measurements of magnetisation for all the compositions were carried out under the applied magnetic field of range ± 10k Oe at room temperature. It is observed that, the magnetic properties such as saturation magnetisation (Ms=16.184 emu/g), remnant magnetisation (Mr=0.38935 emu/g) and coercivity (Hc=23.875 G) values in good agreement with the literature values .
The magnetic structure of spinel ferrite is ferrimagnetic, the magnetic moments of A and B sites are coupled antiparallel to each other. There are twice as many B sites filled, so there is a net magnetic moment equal to the difference between the two sites. The magnetization behaviour of spinel ferrite can be understood in Neel’s model [26, 27]. Zinc-copper ferrite nanoparticles of the composition and cation distribution among the A and B sites will influence the magnetic properties of samples.
According to this, in any ferrite, the magnetic order of tetrahedral clusters (A-site) and octahedral clusters (B-site) was found to be anti-parallel to each other. In this, the A-A and B-B superexchange interaction was predominated by A-B super exchange interaction.
According to Neel’s model, the net magnetic moment of the composition per formula is expressed as:
μB = MB (x) −MA (x)
where MB and MA are the magnetic moments of B and A sub lattices respectively.
Squareness ratio or remnant ratio (Mr/Ms=0.024) of a material is one of the important characteristics which depends on its anisotropy. The values of the squareness ratio represent the random arrangement of uniaxial particles along with the cubic magnetocrystalline anisotropy [28,29].
In the present work, the squareness ratio of Zinc copper ferrite nanoparticles is 0.024 at room temperature. And it has been observed from the literature that the squareness, which indicates the presence of non-interacting single domain particles with cubic anisotropy in the respective compositions . The values of Bohr Magneton (μB) of these samples were also evaluated by using the following Equation (3).
where: Mw is the molecular weight of the sample; Ms is saturation magnetisation.
5585 = β × N [β is Conversion factor (9.27 × 10−21); N is Avogadro’s number].
It is observed that Bohr Magneton values are 1.56. With the research interest, one can modify the compositions of ferrite materials in accordance with squareness ratio (S), for the development of new electromagnetic materials . In the present work, it is observed a clear variation on magnetic properties of Zinc copper ferrite nanoparticles.
The photo-degradation of methylene blue by Zinc copper ferrite nanoparticles is evaluated and the observed absorption spectra are presented in Fig.6 (a). It is clearly shown in the figure that the characteristic absorption peak of the methylene blue (MB) at about 664 nm decreases gradually with increasing exposure time from 0 to 8 hours and almost disappears after 8 hours of irradiation time. This indicates that the MB dye has almost degraded. The photocatalytic performance of the NPs is observed by plotted (C/Co) as a function of time for MB dye and the same is shown in Fig. 6 (b). The presence of Zinc copper ferrite nanocrystal implies the good photo-degradation activity for MB, and no obvious degradation of dye molecules was observed in the darkness, especially, the degradation percentage of MB after 8 hrs. However, Zinc copper ferrite sample exhibited 65%. The dependence of MB photo-degradation on the crystallite size of Zinc copper ferrite nanocrystals is shown in Fig.6 (c). Further, it illustrates that the degradation percentage of MB and their kinetics [31, 32]. Photocatalytic reaction mechanisms for oxidation of MB dye by Zinc copper ferrite are presented in Fig.6 (d). Photocatalytic activities have been improved by Zinc copper ferrite and it can be ascribed from the photo absorptions spreading even up to the visible region and minimizing the electron-hole recombination rate.
Zinc-copper ferrite nanoparticles were prepared through a chemical co-precipitation technique. Structural analysis through powder X-ray diffractometry confirms the spinel phase of all the prepared compounds. TEM also confirms the particle agglomeration and a crystallite size is in agreement with the XRD results. It is observed that the magnetic properties Ms, Mr, and Hc. The squareness ratio (S) the existence of non-conducting domain particles is in accordance with the ions concentration. The obtained Bohr Magneton (μB) values also follow the ions concentration. The synthesized ferrite powder exhibited a good response towards photocatalytic activity for the degradation of MB under visible light irradiation. The optimum conversion achieved was 65%.
CONFLICT OF INTEREST
The authors declare that there is no conflict of interests regarding the publication of this manuscript.