Keywords

1 Introduction

Magnetic nanoparticles are of great technological importance because of their use in magnetic fluid, information storage system, medical diagnostics, and so on. Various preparation techniques have been used for the synthesis of fine particles of ferrites, which exhibit novel properties when compared to their properties in the bulk. Non-conventional methods such as co-precipitation, thermal decomposition, sol-gel and hydrothermal methods have been widely used. Ultra fine ferrite particles can be prepared by chemical co-precipitation method. Auzans et al. [1, 2] have studied the preparation and properties of Mn-Zn ferrite nano particles, which were, used in ionic and surfacted ferrofluids with different degrees of Zn substitution prepared by co-precipitation method. Chandana Rath et al. [3] have reported the dependence on cation distribution of crystallite size, lattice parameter and magnetic properties in nano size Mn-Zn ferrite for different degrees of inversion of Zn substitution prepared by hydrothermal precipitation method.

The use of Mn-Zn ferrite for the preparation of temperature sensitive magnetic fluid by co-precipitation method has already been studied [46]. Co0.2Zn0.8Fe2O4 fine particles have been prepared by chemical co-precipitation method followed by sintering [7]. Control of crystalline size in the nanometer range by the variation of synthesis condition is always a difficult task. It becomes mandatory in the case of ferrofluid preparation using co-precipitation method. In order to prepare ferrofluid having such fine particles, specific size restriction is imposed considering the stability criteria. Co(1−x)MnyZnyFe2O4 (x = 0.9,0.5,0.1 and y = 0.45, 0.25, 0.05.) substituted ferrites were prepared by co-precipitation method have not yet been fully studied like Mn-Zn substituted ferrites. In this paper we report preparation of Me1−xMnyZnyFe2O4 fine particles, where Me = Co2+ with x = 0.9, 0.5, 0.1. Average crystalline size 61 nm by chemical co-precipitation method and the consequent change in their lattice parameter, crystalline size and associated water content due to increase in cobalt concentration were reported.

2 Synthesis and Characterization of Co(1−x)MnyZnyFe2O4 of Nanoparticles

2.1 Synthesis of Cobalt Doped Mn-Zn Ferrites

The cobalt doped ferrite nanoparticles synthesized by co-precipitation depends mostly on parameters such as reaction temperature, pH of the suspension, initial molar concentration etc. [4].Ultra fine particles of Co(1−x)MnyZnyFe2O4 (x = 0.9, 0.5, 0.1 and y = 0.45, 0.25, 0.05.) were prepared by co-precipitating aqueous solutions of CoCl2, MnCl2, ZnCl2 and FeCl3 mixtures respectively in alkaline medium. The mixed solution of CoCl2, MnCl2, ZnCl2 and FeCl3 in their respective stoichiometry (100 ml of 0.1 M CoCl2, 100 ml of 0.45 M ZnCl2, 100 ml of 0.45 M MnCl2 and 100 ml of. 2 M FeCl3 in the case of Co0.1Mn0.45Zn0.45Fe2O4 and similarly for the other values of x) was prepared and kept at 333 K (60 ℃).

This mixture was added to the boiling solution of NaOH (0.63 M dissolved in 1200 ml of distilled water) within 10 s under constant stirring. Nano ferrites are formed by conversion of metal salts into hydroxides, which take place immediately, followed by transformation of hydroxides into ferrites. The solutions were maintained at 358 K (85 ℃) for 1 h. This duration was sufficient for the transformation of hydroxides into spinel ferrite (dehydration and atomic rearrangement involved in the conversion of intermediate hydroxide phase into ferrite) [4]. Sufficient amount of fine particles were collected at this stage by using magnetic separation. These particles were washed several times with distilled water followed by acetone and dried at room temperature.

2.2 XRD

The X-ray diffraction (XRD) patterns of the samples were recorded on a BRUKER-binary V2 (.RAW) powder diffractometer using Cu K(λ = 1.54060 A°) radiation. Slow scans of the selected diffraction peaks were carried out in step mode (step size 0.02°, measurement time 5 s, measurement temperature 323 K (25 °C), standard: Si powder). The crystalline size of the nanocrystalline samples was measured using Debye- Scherrer formula,

$$ {\text{D}}_{{{\text{XRD}}}} = \frac{{0.89\lambda }}{{\beta \cos \theta }}.$$
(1)

2.3 FTIR

FTIR spectra were recorded for the dried samples of Co(1−x)MnyZnyFe2O4 (x = 0.9, 0.5, 0.1 and y = 0.45, 0.25, 0.05.) with Nexus 670 (range 400–4000 cm−1) spectrometer. The dried samples were mixed with KBr and spectra were measured according to transmittance method.

3 Results and Discussions

Generally, XRD can be used to characterize the crystallinity of nanoparticles, and it gives average diameters of all the nanoparticles. The precipitated fine particles were characterized by XRD for structural determination and estimation of crystallite size. XRD patterns were analyzed and indexed using JCPDS. All experimental peaks were matched with (JCPDS #653111) the theoretically generated one and indexed. Analysis of the diffraction pattern using powder-X software [8] confirms the formation of cubic spinel structure for all the samples. All the compositions had a spinel structure. The XRD pattern for Co(1−x)MnyZnyFe2O4 (x = 0.9, 0.5, 0.1 and y = 0.45, 0.25, 0.05.) shown Fig. 1.

Fig. 1
figure 1

X-ray diffraction pattern for Co1−x Mny Zny Fe2O4 with x = 0.9, 0.5, 0.1 and y = 0.45, 0.25, 0.05

The broad XRD lines indicate that the particles are of nanosize range. The particle size was found to decrease from 85 to 41 nm with the increase in cobalt concentration. The crystallite size (DXRD) was estimated by the Debye-Scherrer formula [9] using the full width at half maximum value of the respective indexed peaks. Though all the samples were prepared under identical condition, the crystallite size was not the same for all concentrations (Table 1). This was probably due to the preparation condition followed here, which gave rise to different rate of ferrite formation for different concentrations of cobalt, favoring the variation of crystalline size.

Table 1 The average crystalline size (DaveXR) for Co(1−x)MnyZnyFe2O4

The variation of average crystalline size with the cobalt concentration is given in Fig. 2. Ferrofluids can be conveniently prepared by making use of particles in this size range. The average crystallite size (DaveXR) for Co(1−x)MnyZnyFe2O4 (x = 0.9,0.5,0.1 and

Fig. 2
figure 2

Cobalt concentration versus particle size

y = 0.45,0.25,0.05.) is shown in Table 1. The particle size was confirmed by SEM data (Fig. 3).

Fig. 3
figure 3

SEM images of cobalt doped ferrites

3.1 SEM

3.2 FTIR

From the FTIR spectra for Fe3O4 and for Co(1−x)MnyZnyFe2O4 (x = 0.9,0.5,0.1 and y = 0.45, 0.25, 0.05.), the spectral similarities were observed. The main transmittance frequencies observed in the region 400–4,000 cm−1 of the FTIR spectra for Co(1−x)MnyZnyFe2O4 (x = 0.9, 0.5, 0.1 and y = 0.45, 0.25, 0.05.) are summarized in Table 2.

Table 2 The transmittance frequencies for Co(1−x)MnyZnyFe2O4

The broad feature between 3460.66 and 3031.56 cm−1 is due to O–H stretch (\( \nu_{1} \)), which corresponds to the hydroxyl groups attached by the hydrogen bonds to the iron oxide surface and the water molecules chemically adsorbed to the magnetic particle surface (associated water content) [8]. From these results, it appears that the hydroxyl groups are retained in the samples during the preparation of the uncoated Co(1−x)MnyZnyFe2O 4 . Ghose et al. [7] have reported that the presence of some hydroxyl ions are completely removed when the sample is sintered at temperatures \( \ge \)973 K. The O–H in-plane (\( \nu_{2} \)) and out-of-plane (\( \nu_{3} \)) bonds appear at 1640.02–1509.94 cm−1 and 988.21–986.49 cm1, respectively. The spectrum of the uncoated sample Co(1−x)MnyZnyFe2O4 shows a strong band at \( \nu_{4} \) (635.57–573.51 cm−1) due to Fe3O4 [10]. The transmittance waveband at \( \nu_{4} \)(584.74–583.66 cm−1), which corresponds to the metal-oxygen bonds are considered as the confirmation for the ferrite formation. This is in good agreement with Zins et al. [1, 1114] (Fig. 4).

Fig. 4
figure 4

FTIR spectra for Co(1−x)MnyZnyFe2O4 (x = 0.9,0.5,0.1 and y = 0.45,0.25,0.05)

4 Conclusion

The preparation technique of nano particles has a definite impact on the control of particle size and alteration of magnetic properties. The estimated cations from the product are in comparison with the initial substitution degree, indicating that the preparation procedure favors the formation of only ferrites. The formation of Co (1−x)MnyZnyFe2O4 (x = 0.9, 0.5, 0.1 and y = 0.45, 0.25, 0.05.) was confirmed by the X-ray diffraction. The average crystallite size (DaveXR) decreased when the partial substitution of cobalt increased. The Cobalt doped Mn-Zn ferrite particles can be used to prepare ferro fluids with higher magnetization. FTIR was used to confirm the formation of Fe–O bonds and presence of the associated water content in the samples.