首页> 外文期刊>Metallurgical and Materials Transactions, A. Physical Metallurgy and Materials Science >Nucleation-Controlled Microstructures and Anomalous Eutectic Formation in Undercooled Co-Sn and Ni-Si Eutectic Melts
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Nucleation-Controlled Microstructures and Anomalous Eutectic Formation in Undercooled Co-Sn and Ni-Si Eutectic Melts

机译:过冷Co-Sn和Ni-Si共晶熔体的形核控制显微组织和反常共晶形成

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摘要

Co-20.5 at. pct Sn and Ni-21.4 at. pct Si eutectic alloys have been levitated and undercooled in an electromagnetic levitator (EML) and then solidified spontaneously at different undercoolings. The original surface and cross-sectional morphologies of these solidified samples consist of separate eutectic colonies regardless of melt undercooling, indicating that microstructures in the free solidification of the eutectic systems are nucleation controlled. Regular lamellae always grow from the periphery of an independent anomalous eutectic grain in each eutectic colony. This typical morphology shows that the basic unit should be a single eutectic colony, when discussing the solidification behavior. Special emphasis is focused on the anomalous eutectic formation after a significant difference in linear kinetic coefficients is recognized for terminal eutectic phases, in particular when a eutectic reaction contains a nonfaceted disordered solid solution and a faceted ordered intermetallic compound as the terminal eutectic phases. It is this remarkable difference in the linear kinetic coefficients that leads to a pronounced difference in kinetic undercoolings. The sluggish kinetics in the interface atomic attachment of the intermetallic compound originates the occurrence of the decoupled growth of two eutectic phases. Hence, the current eutectic models are modified to incorporate kinetic undercooling, in order to account for the competitive growth behavior of eutectic phases in a single eutectic colony. The critical condition for generating the decoupled growth of eutectic phases is proposed. Further analysis reveals that a dimensionless critical undercooling may be appropriate to show the tendency for the anomalous eutectic-forming ability when considering the difference in linear kinetic coefficients of terminal eutectic phases. This qualitative criterion, albeit crude with several approximations and assumptions, can elucidate most of the published experimental results with the correct order of magnitude. Solidification modes in some eutectic alloys are predicted on the basis of the present criterion. Future work that may result in some probable errors is briefly directed to improve the model.
机译:Co 20.5 at。 pct Sn和Ni-21.4 at。 pct Si共晶合金已在电磁悬浮器(EML)中悬浮并过冷,然后在不同的过冷度下自发固化。这些凝固样品的原始表面和横截面形态是由独立的共晶菌落组成的,而与熔融物过冷无关,这表明共晶体系的自由凝固中的微观结构是成核控制的。在每个共晶菌落中,规则的薄片总是从独立的异常共晶晶粒的外围生长。这种典型的形态表明,在讨论凝固行为时,基本单位应该是单个共晶菌落。尤其要注意的是,在共晶终末相的线性动力学系数存在显着差异之后,特别是当共晶反应包含无晶面无序固溶体和多晶有序金属间化合物作为终相共晶相后,异常共晶形成就变得异常重要。正是线性动力学系数的显着差异导致了动力学过冷度的显着差异。金属间化合物的界面原子连接中的缓慢动力学引发了两个共晶相解耦生长的发生。因此,为了考虑单个共晶菌落中共晶相的竞争性生长行为,对当前的共晶模型进行了修改,以纳入动力学过冷。提出了产生共晶相解耦生长的临界条件。进一步的分析表明,当考虑末端共晶相的线性动力学系数的差异时,无量纲的临界过冷可能会适合于显示出异常共晶形成能力的趋势。尽管具有一些近似值和假设,但这种定性标准可以用正确的数量级阐明大多数已发布的实验结果。根据目前的标准,可以预测某些共晶合金的凝固方式。可能会导致一些可能的错误的未来工作将直接针对改进模型。

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