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Preparation and Magnetostriction of Tb_(0.22)Dy_(0.48)Ho_(0.35)Fe_2 Alloys

Preparation and Magnetostriction of Tb_(0.22)Dy_(0.48)Ho_(0.35)Fe_2 Alloys
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摘要 Tb0.22Dy0.48Ho0.35Fe2 quaternary alloys are prepared by melting-top casting-annealing process. X-ray diffraction reveals that the alloy is single phase polycrystalline alloy with MgCu2 type cubic Laves phase structure, and (511) preferred orientation occurs in its. The magnetostriction measurements are carried out at room temperature using standard strain gauge technique in magnetic fields up to 400 kA·m-1. The results show that when the magnetic field, H, is 90 kA·m-1, the magnetostriction, λ, of Tb0.22Dy0.48Ho0.35Fe2 quaternary alloys is 260×10-6, and when the H is 210 kA·m-1, the λ is 438×10-6. When the H is 400 kA·m-1, the λ is up to the saturation value, 538×10-6. As compared with TbDyFe ternary alloys, the λ of the quaternary alloy is significantly higher when the H is less than or equal to 210 kA·m-1. When the H is 120 kA·m-1, the λ of the alloy is 333×10-6, 70×10-6 more than the ternary alloy. Research results and mechanism are discussed. Tb0.22Dy0.48Ho0.35Fe2 quaternary alloys are prepared by melting-top casting-annealing process. X-ray diffraction reveals that the alloy is single phase polycrystalline alloy with MgCu2 type cubic Laves phase structure, and (511) preferred orientation occurs in its. The magnetostriction measurements are carried out at room temperature using standard strain gauge technique in magnetic fields up to 400 kA·m-1. The results show that when the magnetic field, H, is 90 kA·m-1, the magnetostriction, λ, of Tb0.22Dy0.48Ho0.35Fe2 quaternary alloys is 260×10-6, and when the H is 210 kA·m-1, the λ is 438×10-6. When the H is 400 kA·m-1, the λ is up to the saturation value, 538×10-6. As compared with TbDyFe ternary alloys, the λ of the quaternary alloy is significantly higher when the H is less than or equal to 210 kA·m-1. When the H is 120 kA·m-1, the λ of the alloy is 333×10-6, 70×10-6 more than the ternary alloy. Research results and mechanism are discussed.
作者 江民红
出处 《Journal of Rare Earths》 SCIE EI CAS CSCD 2007年第S2期198-201,共4页 稀土学报(英文版)
基金 Foundation ite m:Project supported bythe Guangxi Provincial Natural Science Foundation (0575095) Project supported bythe Guangxi"Elec-tronic Information Materials and Devices"Science and Technology Innovation Team
关键词 MAGNETOSTRICTION Tb0.22Dy0.48Ho0.35Fe2 Laves phase low magnetic field magnetostriction Tb0.22Dy0.48Ho0.35Fe2 Laves phase low magnetic field
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参考文献7

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