Elsevier

Thermochimica Acta

Volume 575, 10 January 2014, Pages 64-69
Thermochimica Acta

Nanocrystallization kinetics and magnetic properties of the melt spun amorphous (Fe0.5Co0.5)77Si11B9Cu0.6Nb2.4 alloy

https://doi.org/10.1016/j.tca.2013.10.022Get rights and content

Highlights

Abstract

Kinetics of crystallization in an amorphous (Fe0.5Co0.5)77Si11B9Cu0.6Nb2.4 (at.%) alloy was investigated using differential scanning calorimetry (DSC). Transformed fraction as a function of temperature was obtained by accurate DSC measurement and the experimental data analyzed with Vyazovkin model-free kinetic method. Reconstructed form of the experimental kinetics model, g(α), clearly showed the crystallization mechanism do not belongs to a single model but almost follows the Avrami-Erofe’ev. Magnetic coercivity and hysteresis loss values of the annealed samples at 823 K were 7.5 A m−1 and 1.2 J m−3, compared to 17.1 A m−1 and 37.1 J m−3 for as spun samples. Magnetic measurements show the annealing reduces both coercivity and hysteresis loss at all frequencies.

Introduction

Fe-based amorphous and nanocrystalline alloys have been a research interest since the discovery of Finemet composition (Fe73.5Si13.5B9Cu1Nb3) in 1988 [1]. They show very good magnetic softness, corrosion resistance, and electrical properties and have found wide practical applications [1], [2], [3], [4], [5]. For a suitable chemical composition, nanocrystalline structure could be obtained by proper heat treatment of amorphous precursor [6]. For the Finemet composition, final structure is consist of bcc (Fe)Si or (FeCo)Si (for Co-Finemet) nano-grains randomly dispersed in the remained amorphous matrix [7], [8]. Alloy composition has a crucial role in the formation of nanocrystalline structure. Copper segregates at the initial stage of crystallization that multiplies the nucleation. Niobium with a large atomic radius (0.146 nm) controls the reaction kinetics by retarding the growth of the nano-grains [9], [10], [11], [12]. The composite microstructure of primary crystals distributed in the amorphous matrix makes a great contribution to the magnetic properties. Averaging out of the anisotropies in the nano-grains lowers the overall anisotropy leading to an excellent magnetic softness. This is explained in terms of the random anisotropy model by Herzer [13]. However, controlling the crystallization process and kinetic parameters are essential factors for obtaining the desired structure and properties [14].

Many attempts have been made to improve these materials by optimizing the alloy compositions [15], [16], heat treatment conditions [17], or by adding the alloying elements [18], [19], [20]. Modifying the chemical composition is a way to tune the structure by a change in the transformation kinetics. For example, the percentage of copper in the alloy controls the size and distribution of nano-grains in the Finemet alloys [15], or substitution of iron by cobalt reduces the crystallization onset temperature [18]. For Finemet-type alloys, partial replacement of iron with cobalt also plays a crucial role in broadening its applications, which requires much higher performance of soft magnetic materials. Accordingly, a large number of research results have proven the improvement in high-temperature and high frequency magnetic properties of the Co-Finemet alloys [21], [22], [23]. The incorporation of cobalt is not only expected to improve ferromagnetic properties but also to play a dual role as a nucleating element in place of copper in Finemet systems [12].

Since, the kinetic parameters are important factors determining the structure and properties of nano-crystalline alloy, present work aims to study the kinetics of cobalt containing Finemet alloy (Fe0.5Co0.5)77Si11B9Cu0.6Nb2.4 (at.%). The alloy composition derived by replacing of iron with cobalt into the modified Finemet composition of Fe77Si11B9Nb2.4Cu0.6 [24]. According to Ohnuma et al. [15], the modified composition has an improved magnetic flux density in comparison to the original composition Fe73.5Si13.5B9Cu1Nb3. Vyazovkin isoconversional method [25], [26], [27] was selected for kinetic calculations due to its accuracy and reliability.

Section snippets

Experimental

Ingot of master alloy (Fe0.5Co0.5)77Si11B9Cu0.6Nb2.4 (at.%) were prepared by arc melting under the protective argon atmosphere. Amorphous ribbons with a cross section of 0.02 mm × 1.00 mm were prepared by melt spinning technique. Actual composition was checked by inductivity coupled plasma (ICP) analysis. The amorphous nature of the ribbons was analyzed using X-ray diffractometer (Philips PW 1830) with a Co-Kα (1.78897 Å) radiation. In order to investigate the structural transformations, amorphous

Results and discussion

Typical DSC curve for the heating cycle of as quenched sample at the heating rate of 20 K min−1 is present in Fig. 1. The figure involves two exothermal peaks; the first peak corresponds to the crystallization of (FeCo)-Si grains (primary crystallization), and the second one is related to the formation of boride phases. Onset and the peak temperatures are marked on the curves. Area under the peak is directly related to the transformed fraction and used for calculation of transformed fraction

Conclusion

Magnetic properties and the kinetics of crystallization in cobalt containing Finemet alloy (Fe0.5Co0.5)77Si11B9Cu0.6Nb2.4 (at.%) was investigated. Comparisons of the results with those obtained for similar composition confirm the improvement in high frequency magnetic properties by cobalt addition. Kinetic results, based on accurate DSC measurements, show the activation energy for crystallization is a variable as a function of transformed fraction, implies a complex multistage reaction. The

Acknowledgements

The authors gratefully acknowledge the financial and other support of this research, provided by the Islamic Azad University, Eslamshahr Branch, Tehran, Iran.

References (36)

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