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Viscous flow and crystallization of bulk metallic glass-forming liquids.

机译:粘性流动和大块金属玻璃形成液体的结晶。

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摘要

An experimental setup was designed and implemented to measure the flow behavior of liquids in the viscosity range from 10−1 Pa s to 104 Pa s. The viscosity of the Zr41.2 Ti13.8Cu10.0Ni12.5Be22.5 (V1) bulk metallic glass forming alloy was measured over a temperature range from 927 K to 1173 K. At the liquidus temperature, the viscosity is 2.3 Pa s, which is about three orders of magnitude larger than the viscosity of a pure metallic liquid. The free volume theory as formulated by Cohen and Grest describes the temperature dependence of the viscosity of V1 over 14 orders in magnitude.; The high viscosity of V1 above the liquidus temperature stabilizes the liquid against convective flow due to temperature gradients and allows for diffusion experiments in the equilibrium liquid. The temperature dependence of the diffusivity of large atoms like Al or Au scales with the viscosity. The time scales obtained from the viscosity measurements suggest that above the calorimetric glass transition region the diffusion of small and medium sized atoms is governed by thermally activated jumps.; Liquid V1 could be successfully supercooled inside high purity graphite crucibles without changing the stability of the supercooled liquid with respect to crystallization compared to levitated samples. The sluggish kinetics that are reflected in the high viscosity in the supercooled liquid state contribute significantly to the good glass forming ability of the alloy. The critical cooling rate is about 1 K/s.; The onset of crystallization under isothermal conditions as well as upon heating from the amorphous state was studied in detail. The critical heating rate to bypass crystallization was measured to be 200 K/s and the difference between the critical cooling and critical heating rate can be qualitatively understood in the framework of nucleation and growth.; However, the observed deviations from classical steady state nucleation behavior indicate a more complex crystallization mechanism. Rheological and crystallization studies at constant shear rate suggest that changes in the morphology of the supercooled liquid of V1 occur as a precursor of crystallization.
机译:设计并实施了一个实验装置,以测量粘度范围为10 -1 Pa s到10 4 Pa s的液体的流动行为。 Zr 41.2 Ti 13.8 Cu 10.0 Ni 12.5 Be 22.5 的粘度( V1)块状金属玻璃成形合金是在927 K到1173 K的温度范围内测量的。在液相线温度下,粘度为2.3 Pa s,比纯金属液体的粘度大约三个数量级。 Cohen和Grest提出的自由体积理论描述了V1粘度在14个数量级以上的温度依赖性。 V1在液相线温度以上的高粘度使液体抵抗温度梯度引起的对流流动,并允许在平衡液体中进行扩散实验。大原子(如Al或Au)的扩散率随温度的变化随粘度变化。从粘度测量获得的时间尺度表明,在量热玻璃化转变区域上方,中小原子的扩散受热活化跃迁控制。与悬浮样品相比,液体V1可以成功地在高纯度石墨坩埚中过冷,而不会改变过冷液体在结晶方面的稳定性。在过冷液态下的高粘度反映出的缓慢动力学显着地促进了合金的良好玻璃形成能力。临界冷却速度约为1 K / s。详细研究了在等温条件下以及从无定形状态加热时结晶的开始。旁路结晶的临界加热速率经测量为200 K / s,可以在成核和生长的框架内定性地理解临界冷却速率和临界加热速率之间的差异。但是,观察到的与经典稳态成核行为的偏差表明了更复杂的结晶机理。在恒定剪切速率下的流变和结晶研究表明,V1过冷液体的形态变化是结晶的前兆。

著录项

  • 作者

    Masuhr, Andreas.;

  • 作者单位

    California Institute of Technology.;

  • 授予单位 California Institute of Technology.;
  • 学科 Engineering Materials Science.; Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 1999
  • 页码 104 p.
  • 总页数 104
  • 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 11:47:58

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