13 research outputs found

    Measurements of Magnetocaloric Effect in LaFe11.14Co0.66Si1.2xAlxLaFe_{11.14}Co_{0.66}Si_{1.2-x}Al_{x} (x=0.1, 0.2, 0.3) Alloys

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    In the present work, phase constitution and thermomagnetic properties of LaFe11.14Co0.66Si1.2xAlxLaFe_{11.14}Co_{0.66}Si_{1.2-x}Al_{x} (where x = 0.1, 0.2, 0.3) alloys were investigated. Ingot samples were obtained by arc-melting under the low pressure of Ar atmosphere. Subsequently samples were annealed at 1323 K for 15 days. X-ray diffraction of all samples revealed coexistence of two crystalline phases dominant La(Fe,Si)13La(Fe,Si)_{13}-type and minor bcc α -Fe. Furthermore, the magnetic measurements at various temperatures allowed to study the Curie temperature, magnetic entropy changes and relative cooling power

    Measurements of Magnetocaloric Effect in LaFe 11.14

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    In the present work, phase constitution and thermomagnetic properties of LaFe11.14Co0.66Si1.2xAlxLaFe_{11.14}Co_{0.66}Si_{1.2-x}Al_{x} (where x = 0.1, 0.2, 0.3) alloys were investigated. Ingot samples were obtained by arc-melting under the low pressure of Ar atmosphere. Subsequently samples were annealed at 1323 K for 15 days. X-ray diffraction of all samples revealed coexistence of two crystalline phases dominant La(Fe,Si)13La(Fe,Si)_{13}-type and minor bcc α -Fe. Furthermore, the magnetic measurements at various temperatures allowed to study the Curie temperature, magnetic entropy changes and relative cooling power

    Phase Structure in Fe-Cr-Co Permanent Magnet Alloy

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    The Mössbauer spectroscopy, electron microscopy and magnetization measurements were used in order to describe structural changes in Fe58.75\text{}_{58.75}Cr29.4\text{}_{29.4}Co11.85\text{}_{11.85} alloy during magnetic hardening. Multiphase structure was found in alloy with best magnetic properties

    Effect of Ga Addition on Structure and Magnetic Properties of the LaFe11.14Co0.66Si1.2xGaxLaFe_{11.14}Co_{0.66}Si_{1.2-x}Ga_{x} (x=0.1, 0.2, 0.3) Alloys

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    In the present work, the phase constitution and magnetic properties of the LaFe11.14Co0.66Si1.2xGaxLaFe_{11.14}Co_{0.66}Si_{1.2-x}Ga_{x} (where x=0.1, 0.2, 0.3) alloys, were investigated. It was revealed that increase of Ga content in the alloy composition causes the rise of lattice parameter of the La(Fe,Si)13La(Fe,Si)_{13}-type phase, which causes increase of the Curie temperature. However, the increase of Ga addition leads to decrease of magnetocaloric effect

    Ordering of alfa-FeCo phase in the nanocrystalline Fe83-xCoxNb3B13Cu1 (x = 6, 25 or 41.5) alloy

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    The microstructure and ordering of alfa-FeCo phase of the nanocrystalline Fe83 xCoxNb3B13Cu1 (x = 6, 25 or 41.5) alloys were investigated. We have stated that á-FeCo phase is atomically ordered in the Fe83 xCoxNb3B13Cu1 (x = 25 or 41.5) samples crystallized by the heat treatment in a furnace. However, after flash annealing (by current or laser) that phase is disordered. Moreover, we have found that Co concentration in the crystalline alfa-FeCo phase strongly depends on Co content in the as-quenched ribbons. The annealing conditions influence also the grain diameter of the crystalline phase. In the nanocrystalline alloys obtained by a flash annealing of the amorphous ribbons finer grains are present

    Effect of Al content on the order of phase transition and magnetic entropy change in LaFe11Co0.8(Si1xAlx)1.2\mathrm{LaFe_{11}Co_{0.8}(Si_{1-x}Al_{x})_{1.2}} alloys

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    The comparative studies of the effect of partial substitution of Al by Si on the structure and magnetic entropy change in LaFe11_{11}Co0.8_{0.8}(Si1x_{1-x}Alx_{x})1.2_{1.2} alloys produced by arc-melting followed by long time annealing at 1323 K were performed. The X-ray diffraction analysis revealed almost single phase composition of annealed samples. The high intensity synchrotron radiation was used for studying the thermal evolution of lattice constant of the La(Fe,Co,Si)13_{13} phase. Furthermore, calculations of temperature dependences of Landau coefficients were used to reveal changes in the character of phase transformation at around the Curie temperature
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