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LIQUIDUS SURFACE AND MELTING DIAGRAM OF THE TERNARY Ni–Ti–Zr SYSTEM IN RICH IN NICKEL AREA OF CONTENTS

机译:富含镍含量的富含三元NI-TI-ZR系统的液相和表面和熔化图

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摘要

Multicomponent alloys based on Ni–Ti system known as high-temperature corrosion-resistant materials that have an attractive combination of mechanical, chemical and physical properties and are used as structural materials and functional diversification purposes. The ternary alloys of the Ni–Ti–Zr system attract attention, in particular, due to their ability to crystallize in an amorphous state at relatively low cooling rates, that is, they have the ability to form so-called bulk amorphous alloys. Literature data concern phase equilibria in the ternary system are rather limited. The system was studied in temperature interval from 700 °С to the liquidus surface in the concentration range from 0 to 50% (at.) Ni by Eremenko with co-authors (1988-1992). There is the only work in the solid / liquid equilibria region with a nickel content of more than 50 % (at.) – Liu X.J. et al (2015) – isothermal sections at 1000 and 1200 °С, that does not give an idea about crystallization processes. Besides in our previous work the solidus surface projection was constructed. In present work we present the results about the phase equilibria in the melting / crystallization region in the concentration range from 75 to 100 % (at.) Ni. The arc-melting alloys were studied by scanning electron microscopy with electron probe microanalysis (SEM / EPMA) and differential thermal analysis (DTA). Based on the results of the experimental study the liquidus surface projection and the melting diagram of the ternary one Ni–Ti–Zr system in the region Ni–Ni3Ti–Ni7Zr2 are constructed. The liquidus surface consists of four fields of primary crystallization – solid solutions of ⟨Ni⟩, ⟨Ni3Ti⟩, ⟨Ni5Zr⟩ and ⟨Ni7Zr2⟩. The liquidus temperature decreases from the bounding binary systems to the ternary one to a minimum at 1182 °С at the point Ni84.5Ti7.9Zr7.6 of the ternary eutectics composition LЕ1 ↔ ⟨Ni⟩ + ⟨Ni3Ti⟩ + ⟨Ni5Zr⟩. The invariant point coordinates on liquidus surface were established: LU1 + ⟨Ni7Zr2⟩ ↔ ⟨Ni5Zr⟩ + ⟨Ni3Ti2⟩ – Ni83.0Ti8.5Zr8.5, 1190 °С; lе3 ↔ Ni + Ni5Zr – Ni87.4Ti4.5Zr8.1, 1187 °С; lе2 ↔ Ni3Ti + Ni7Zr2 – Ni76.3Ti13.2Zr10.5, 1288 °С.
机译:基于Ni-Ti系统的多组分合金,称为高温腐蚀材料,具有机械,化学和物理性质的有吸引力组合,并用作结构材料和功能多样化目的。 Ni-Ti-Zr系统的三元合金尤其引起注意,由于它们以相对低的冷却速率在非晶态结晶的能力,即它们具有形成所谓的散装非晶合金的能力。文学数据涉及三元系统中的相平衡相当有限。通过Eremenko与共同作者(1988-1992),在浓度范围内以700°С的温度间隔从700°С中的温度间隔进行研究,浓度范围为0至50%(AT。)NI。固体/液体均衡区域唯一有效,镍含量超过50%(at。) - liu x.j.等(2015) - 等温截面在1000和1200°С,这不给出关于结晶过程的想法。此外,在我们之前的工作中,构造了固体表面投影。在目前的工作中,我们介绍了浓度范围内的熔融/结晶区域中的相平衡的结果,从75-100%(AT。)Ni。通过用电子探针微透视(SEM / EPMA)和差分热分析(DTA)扫描电子显微镜来研究弧形熔融合金。基于实验研究的结果,构建了地区Ni-Ni3Ti-Ni7zR2中的三元Ni-Ti-Zr系统的液相表面突起和熔化图。液相液面由四个初级结晶 - 固体溶液的四个领域组成,Ni,Ni3Ti⟩,Ni5Zr和⟨Ni7zR2的固体溶液。在三元共晶组合物的点Ni84.5Ti7.9ZR7.6的点Ni84.5Ti7.9ZR7.6,液相液从边界二元系统从界定的二元体系中的液体温度降低至最小1182°O .1↔↔ni⟩+⟨ni3ti⟩+⟨ni5zr⟩。确定液体表面上的不变点坐标:Lu1 +⟨ni7zr2⟩⟩↔ni5zr⟩+⟨ni3ti2⟩ - ni83.0ti8.5zr8.5,1190°С; lе3↔ni + ni5zr - ni87.4ti4.5zr8.1,1187°С; Lе2↔NI3TI+ NI7ZR2 - NI76.3TI13.2ZR10.5,1288°С。

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