首页> 外文期刊>International Journal of Modern Physics, B. Condensed Matter Physics, Statistical Physics, Applied Physics >Microstructure and magnetostrictive properties of epoxy-bonded Tb_(1?x)Nd_x(Fe_(0.8)Co_(0.2))_(1.93)(0.20 ≤ x ≤ 0.75) composites
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Microstructure and magnetostrictive properties of epoxy-bonded Tb_(1?x)Nd_x(Fe_(0.8)Co_(0.2))_(1.93)(0.20 ≤ x ≤ 0.75) composites

机译:环氧键合Tb_(1?x)Nd_x(Fe_(0.8)Co_(0.2))_(1.93)(0.20≤x≤0.75)复合材料的微观结构和磁致伸缩性能

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摘要

An epoxy-resin bonding route was used to produce composite rods of the highly magnetostrictive alloys Tb_(1?x)Nd_x(Fe_(0.8)Co_(0.2))_(1.93) (0.20 ≤ x ≤ 0.75). The structure, spin configuration, magnetostriction and particle size are investigated by means of X-ray diffraction (XRD), a standard strain technique and scanning electron microscope (SEM). The epoxy-bonded 0–3 type and pseudo 1–3 type composites are successfully fabricated, respectively. XRD analysis shows that the easy magnetization direction (EMD) for the alloy of x = 0.20 lies along h111i axis. The magnetic curing field makes the particles align as a particulate chain and also causes the particles rotating along its EMD direction. The pseudo 1–3 type epoxy-bonded composite has a larger magnetostriction than that of the 0–3 type composite, which can be attributed to the larger magnetostriction coefficient λ_(111), EMD lying along <111> direction, the <111>-textured orientation and the chain structure. A large saturation magnetostriction (λ_(0S) ~ 570 ppm) is achieved for the 1–3 type epoxy/Tb_(0.35)Nd_(0.65)(Fe_(0.8)Co_(0.2))_(1.93) composite (about 150–250 μm, 10 kOe), which approaches 70% of its monolithic alloy. Furthermore, it only contains 27 vol.% alloy particles in the insulating epoxy matrix and performs a low magnetic anisotropy, which could make it technologically interesting for the field of Nd-containing magnetostrictive materials.
机译:使用环氧树脂结合路线生产高磁致伸缩合金Tb_(1?x)Nd_x(Fe_(0.8)Co_(0.2))_(1.93)(0.20≤x≤0.75)的复合棒。通过X射线衍射(XRD),标准应变技术和扫描电子显微镜(SEM)研究了结构,自旋构型,磁致伸缩和粒径。分别成功地制造了环氧键合的0-3型和伪1-3型复合材料。 XRD分析表明,x = 0.20的合金的易磁化方向(EMD)沿h111i轴。磁固化场使颗粒排列成颗粒链,还使颗粒沿其EMD方向旋转。伪1-3型环氧粘结复合材料的磁致伸缩比0-3型复合材料的磁致伸缩大,这可以归因于较大的磁致伸缩系数λ_(111),沿<111>方向的EMD位于<111>纹理定向和链结构。 1–3型环氧树脂/Tb_(0.35)Nd_(0.65)(Fe_(0.8)Co_(0.2))_(1.93)复合材料可实现较大的饱和磁致伸缩(λ_(0S)〜570 ppm)。 250μm,10 kOe),接近其整体合金的70%。此外,它在绝缘环氧树脂基质中仅包含27%(体积)的合金颗粒,并且具有低的磁各向异性,这可能使其在含Nd磁致伸缩材料领域具有技术吸引力。

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