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Preparation and characterization of bulk amorphous and nanostructured iron-40 nickel-40 phosphorus-14 boron-6 alloys.

机译:块状非晶态和纳米结构铁40镍40磷14硼6合金的制备和表征。

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摘要

The reduced glass transition temperature of ferromagnetic Fe40Ni 40P14B6 alloy is 0.57 and it implies moderate glass formability. In the past thirty years this alloy system has been investigated extensively. By means of some novel methods, bulk amorphous and nanostructured Fe40Ni40P14B6 alloys had been prepared in our experiment and their properties had been studied in details.; By means of a rapid quenching technique, ferromagnetic bulk amorphous Fe40Ni40P14B6 alloy rods with a diameter of ∼1.2 mm were prepared. When a fluxing technique was also employed, amorphous rods with a diameter as large as ∼2.5 mm were synthesized. The corresponding critical cooling rate Rc for the glass formation Fe40Ni40P14B6, according to earlier reports, is estimated to be on the order of 102 K s −1. The measurements on the as-prepared specimens indicate that the thermal stability and magnetic properties of bulk Fe40Ni 40P14B6 amorphous rods prepared in our work are comparable to those obtained from thin Fe40Ni40P 14B6 glassy ribbons prepared at a cooling rate of 10 5 K s−1. Small differences between them can be explained by the reason that the atom arrangement of bulk Fe40Ni 40P14B6 amorphous specimens prepared at a cooling rate of ∼102 K s−1 in our work is closer to the ideal glass state than that of the specimens prepared by means of the melt-spinning technique.; It was pointed out that when a molten eutectic alloy is undercooled to a temperature T that is substantially below its liquidus T1, it will undergo metastable liquid state spinodal decomposition (LSD) to become a system of intertwining liquid networks of wavelength λ. The larger undercooling will result in the smaller λ. When the undercooling is large enough, subsequent crystallization transforms the system into a nanostructure, characterised as bulk, pore-free, and of narrow grain-size distribution. Based on the above principles, bulk nanostructured Fe40Ni40P 14B6 alloy ingots of diameter 3 ∼ 5 mm had been synthesized in our experiment. The molten Fe40Ni40P14B 6 alloy was purified by means of the fluxing technique and thus a large undercooling could be achieved. For ΔT > 260 K, the microstructure of the undercooled specimen had exhibited LSD in the undercooled liquid state. The microstructure could be described as two intertwining networks with small grains dispersed in them. For ΔT > 290 K, the overall microstructure of the specimen changed into a granular morphology. The average grain sizes of the small and large grains are ∼30 nm and ∼80 nm, respectively.
机译:铁磁性Fe 40 Ni 40 P 14 B 6 合金的降低的玻璃化转变温度为0.57,表明温度适中玻璃成形性。在过去的三十年中,对该合金体系进行了广泛的研究。通过一些新颖的方法,已经形成了块状非晶态和纳米结构的Fe 40 Ni 40 P 14 B 6 合金在我们的实验中制备了它们,并对其性质进行了详细的研究。通过快速淬火技术,铁磁块状非晶Fe 40 Ni 40 P 14 B 6 合金棒直径约为1.2毫米。当还使用助熔剂技术时,合成了直径约2.5mm的非晶棒。 Fe 40 Ni 40 P 14 B 6形成的玻璃的相应临界冷却速率R c 根据先前的报告,估计约为10 2 K s -1 。对所制备试样的测量表明,块状Fe 40 Ni 40 P 14 B 6的热稳定性和磁性能在我们的工作中制备的非晶棒与从薄Fe 40 Ni 40 P 14 B 6 < / sub>玻璃带,其冷却速率为10 5 K s -1 。两者之间的微小差异可以解释为:Fe 40 Ni 40 P 14 B 6 的原子排列在我们的工作中,以〜10 2 K s -1 的冷却速率制备的sub>非晶态样品比通过以下方法制备的样品更接近理想玻璃态:熔纺技术。有人指出,当熔融的共晶合金被过冷至实质上低于其液相线T 1 的温度T时,它将经历亚稳态的液态旋节线分解(LSD),成为相互缠绕的液体体系。波长为λ的网络。过冷度越大,λ越小。当过冷度足够大时,随后的结晶会将系统转变为纳米结构,其特征是体积大,无孔且晶粒尺寸分布窄。基于上述原理,制备了直径为3〜3的块状纳米Fe 40 Ni 40 P 14 B 6 合金锭在我们的实验中合成了5毫米。熔融的Fe 40 Ni 40 P 14 B 6 合金通过助熔技术进行纯化,因此可以实现较大的过冷度。当ΔT> 260 K时,过冷试样的微观结构在过冷液态下表现出LSD。微观结构可以描述为两个相互缠绕的网络,其中散布着小颗粒。当ΔT> 290 K时,样品的整体微观结构变为颗粒状。小晶粒和大晶粒的平均晶粒尺寸分别为〜30 nm和〜80 nm。

著录项

  • 作者

    Li, Qiang.;

  • 作者单位

    Chinese University of Hong Kong (People's Republic of China).;

  • 授予单位 Chinese University of Hong Kong (People's Republic of China).;
  • 学科 Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 2002
  • 页码 127 p.
  • 总页数 127
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 工程材料学;
  • 关键词

  • 入库时间 2022-08-17 11:46:38

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