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Isotropic rare earth based hard magnets through non-equilibrium processing.

机译:通过非平衡处理的各向同性稀土基硬磁铁。

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The aim of this thesis was to understand better the relationship of hard magnetic properties to the microstructure and use this knowledge to design a better magnet.;The first project was focused on the development of isotropic Pr 9Fe85B6 ribbons with enhanced remanence, high coercivity and high (BH)max. The optimization was achieved by adjusting the composition, controlling the microstructure and processing parameters. The crystal structure in all the samples studied was found to consist of a fine mixture of hard phase 2:14:1 and soft alpha-Fe phase. In all the samples the optimum (BH)max obtained was in the optimally quenched ribbons. Annealing did improve the magnetic properties but did not exceed the highest (BH)max value obtained in the optimally quenched ribbons. Small additions of Tb and Co were found to improve the magnetic properties. The properties were optimized by first adjusting the wheel speed and then the ejection temperature of melt. A maximum (BH)max 21 MGOe and a remanence of 117 emu/g were obtained in the ribbons spun at 18 m/s and ejected at a temperature of 1360°C with a average grain size of 20 nm. This investigation suggests that a proper combination of composition and processing parameters is essential for the optimum (BH)max value for the Pr-Fe-B magnets.;The second project was focused on the development of a single phase nanocrystalline Sm2(Co, Fe)17 magnets. The magnetic properties such as coercivity and energy product were optimized via the design of composition, control of melt-spinning parameters and heat treatment. The effect of non magnetic elements like Si, B, addition on the Sm(Co, Fe, M)z alloys were investigated. The effect of C addition on the Smx(Co 1-yMy)100-x-zCz series alloys where, M= Fe or Fe+Mn, X=10-15, Y= 0-0.375, Z= 0-6 were studied thoroughly. It is observed that the crystal structure of Sm(Co0.75Fe0.25 )7, Sm(Co0.65Fe0.25Si0.1) 7 and Sm(Co0.65Fe0.25Si0.05B0.05 )8 alloy ribbons spun at low wheel speed shows the presence of 1:5 and 2:17 phase and the metastable 1:7 phase for high wheel speed. It is observed that C suppressed the formation of the stable 2:17 structure in favor of the disordered 1:7 phase. Addition of Si and B, C leads to the development of equiaxed finer grains. C may have act as grain growth inhibitor in the Sm-(Co-Fe)- C ribbons Microstructure refinement with the precipitation of RCoC2 carbides was observed in the C added ribbons. The carbon addition enhances the overall magnetic properties.;The 3rd project was focused on the investigation of giant intrinsic magnetic hardness in Sm(Co0.45,Fe0.15,Cu0.4) 5 alloys and determine its dependence on grain / particle size. Melt-spinning and high energy ball milling was used to prepare sample with different grain size (6-500 nm). A single phase 1:5 structure was observed in both the ribbons and milled powders of the Sm(Co0.45,Fe0.15,Cu0.4 )5 alloy. The maximum coercivity obtained was 21 kOe for ribbons spun at 50 m/s (70 nm) and 15 kOe for the powders milled for 15 min (15 nm). Low temperature annealing of ribbons with large grain size > 500 nm for 133 h increases the coercivity to 44 kOe similar like bulk. The effect of low temperature annealing of ribbons with the coarse grain structure (> 70 nm) was the increasing of coercivity, it also increased the Curie temperature of 1: 5 phase and resistivity. The effect of low temperature annealing on the coercivity of high energy milled powders with a smaller grain size (< 70 nm) was different from the ribbons. The maximum coercivity of 21 kOe was obtained for 3h milled powders annealed at 400°C for 1 h. However, after longer annealing the coercivity decreases and this is different behavior from bulk. The effect of annealing on the homogenized crushed powders (>140nm) was more like bulk, even after annealing for 50 h at 400°C coercivity obtained was 38.48 kOe and increasing. (Abstract shortened by UMI.).
机译:本论文的目的是更好地理解硬磁性能与显微组织之间的关系,并以此知识设计出更好的磁体。第一个项目的重点是开发具有增强剩磁,高矫顽力和高强度的各向同性Pr 9Fe85B6薄带。 (BH)最大通过调节成分,控制微观结构和加工参数来实现优化。发现所有研究样品的晶体结构均由硬质相2:14:1和软质α-Fe相的精细混合物组成。在所有样品中,获得的最佳(BH)max在最佳淬火带中。退火确实改善了磁性能,但没有超过在最佳淬火带中获得的最高(BH)max值。发现少量添加Tb和Co可以改善磁性。通过首先调节轮速,然后调节熔体的喷射温度来优化性能。在以18 m / s旋转的碳带中获得了最大(BH)max 21 MGOe和剩磁117 emu / g,并在1360°C的温度下喷射,平均晶粒尺寸为20 nm。这项研究表明,适当组合成分和加工参数对于Pr-Fe-B磁体的最佳(BH)max值至关重要。 )17个磁铁。通过成分设计,熔体纺丝参数控制和热处理优化了矫顽力和能量积等磁性能。研究了非磁性元素,如Si,B,添加对Sm(Co,Fe,M)z合金的影响。研究了C添加对Smx(Co 1-yMy)100-x-zCz系列合金的影响,其中M = Fe或Fe + Mn,X = 10-15,Y = 0-0.375,Z = 0-6彻底观察到低轮转速下旋转的Sm(Co0.75Fe0.25)7,Sm(Co0.65Fe0.25Si0.1)7和Sm(Co0.65Fe0.25Si0.05B0.05)8合金带的晶体结构显示了高轮速时存在1:5和2:17相位以及亚稳1:7相位。观察到C有利于无序的1:7相抑制了稳定的2:17结构的形成。 Si和B,C的添加导致等轴细晶粒的发展。 C可能在Sm-(Co-Fe)-C碳带中起晶粒生长抑制剂的作用在添加C的碳带中观察到随着RCoC2碳化物沉淀的微观组织细化。碳的添加增强了整体磁性能。第三项目着眼于研究Sm(Co0.45,Fe0.15,Cu0.4)5合金的巨大固有磁硬度,并确定其对晶粒/粒径的依赖性。熔融纺丝和高能球磨用于制备具有不同晶粒尺寸(6-500 nm)的样品。在Sm(Co0.45,Fe0.15,Cu0.4)5合金的薄带和粉末中均观察到单相1:5结构。对于以50 m / s(70 nm)旋转的色带,获得的最大矫顽力为21 kOe,对于研磨15分钟(15 nm)的粉末,则为15 kOe。大晶粒尺寸> 500 nm的薄带的低温退火133 h可将矫顽力提高到44 kOe,类似于体积。带粗晶粒结构(> 70 nm)的带材进行低温退火的效果是矫顽力的增加,还提高了居里温度(1:5)和电阻率。低温退火对具有较小晶粒尺寸(<70 nm)的高能研磨粉的矫顽力的影响与薄带不同。对于在400°C退火1h的3h研磨粉末,获得的最大矫顽力为21 kOe。但是,经过较长时间的退火后,矫顽力降低了,这与本体不同。退火对均质粉碎粉末(> 140nm)的影响更像松散,即使在400°C退火50小时后,所获得的矫顽力也为38.48 kOe,并且还在增加。 (摘要由UMI缩短。)。

著录项

  • 作者

    Sultana, Dilara.;

  • 作者单位

    University of Delaware.;

  • 授予单位 University of Delaware.;
  • 学科 Condensed matter physics.
  • 学位 Ph.D.
  • 年度 2010
  • 页码 213 p.
  • 总页数 213
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-17 11:37:35

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