42 research outputs found
Structure and Microstructure Properties of Ball Milled Fe-Zn
Nanocrystalline Fe10 %Zn and Fe30 %Zn alloys have been prepared from pure elemental powders by
mechanical alloying processing in a high energy planetary ball-mill. Microstructural, structural, and magnetic
characterizations of the powders were investigated by X-ray diffraction, and vibrating sample magnometer.
The crystallite size reduction to the nanometer scale is accompanied by an increase in the atomic
level strain. The reaction between Fe and Zn leads to the formation of a bcc Fe(Zn) solid solution with a
lattice parameter close to (0.2912 nm for Fe30 %Zn and 0,2885 nm for Fe10 %Zn) after 5 h of milling. The
complete dissolution of the elemental Zn powders in the a-Fe lattice gives rise to the formation of a highly
disordered Fe(Zn) solid solution, where a-Fe(Zn) nanograins have a crystallite size of (229,29 Å for
Fe10 %Zn (24 h) 30,09 Å for Fe30 %Zn (24 h), on prolonged milling time. The coercivity and magnetization
values are 18,90 (Fe10 %Zn)Oe and 26,59 (Fe30 %Zn) emu/g, respectively, after 24 h of milling.
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Effect of Al Substitution on Structural, Magnetic, and Magnetocaloric Properties of Er6Fe23−xAlx (x = 0 and 3) Intermetallic Compounds
The structural, magnetic, and magnetocaloric properties of Er6Fe23−xAlx (x = 0 and 3) intermetallic compounds have been studied systematically. Samples were prepared using the arc furnace by annealing at 1073 K for one week. Rietveld analysis of XRD shows the formation of pure crystalline phase with cubic Fm-3m structure. Refinement results show that the unit cell volume decreases with increasing Al content. The Curie temperature Tc of the prepared samples was found to be strongly dependent on the aluminum content. This reduces magnetization and the ferrimagnetic phase transition temperature (Tc) from 481 K (for x = 0) to 380 K (for x = 3), is due to the substitution of magnetic element (Fe) by non-magnetic atoms (Al). With the increase of the Al content, a decrease in the values of magnetic entropy is observed. The magnitude of the isothermal magnetic entropy (|∆SM|) at the Tc decreases from 1.8 J/kg·K for x = 0 to 0.58 J/kg·K for x = 3 for a field change 14 kOe. Respectively, the relative cooling power (RCP) decreases with increasing Al content reaching 42 Jkg−1 for x = 0 to 28 Jkg−1 for x = 3
Magnetic and Structural Properties of the Nanostructured Cu50Ni50 Powders
International audienc
Structure, Magnetocaloric Effect and Critical Behaviour in Ni50Mn30(Sn,In)20 Heusler Alloys
International audienc
Structural, magnetic and on magnetocaloric properties near the paramagnetic to ferromagnetic phase transition in La 0.5 □ 0.1 Ca 0.4 MnO 3 oxide
International audienc
Investigation of the critical behavior and magnetocaloric properties in the nanocrystalline CuNi powders
International audienc
Phase transformations and magnetic properties of ball-milled Fe–6P–1.7C powders
International audienc
X-ray diffraction, Mössbauer spectrometry and thermal studies of the mechanically alloyed (Fe 1−x Mn x ) 2 P powders
International audienc
Effect of the Mn/Fe Ratio on the Microstructure and Magnetic Properties in the Powder Form (Fe1−x Mn x )2P System
International audienc
Critical behavior, magnetic and magnetocaloric properties of melt-spun Ni50Mn35Sn15 ribbons
International audienc