钛合金中正交马氏体晶体结构的一般模型

S. Demakov, I. Kylosova, S. Stepanov, M. Bönisch
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引用次数: 2

摘要

本文提出了一种新的统一的方法来描述Ti合金中正交马氏体(α”)的晶体结构与化学成分无关。通过对基本四面体结构单元采用一种简单但极具指导性的实心球模型,将β↔α " /α '马氏体相变中涉及的晶体结构分为几种中间形态。重要的是,引入了一个新的度量,δ,它明确地描述了正交单元胞内的原子位置,这取决于单元胞的几何形状。此外,仅使用相对量来描述单元胞的几何形状和原子位置,使得本文开发的方法与合金含量无关。通过这种方式,消除了通常建议的α”结构度量的缺点。随后,基于实验测量的单元胞参数,该新方法被应用于分析和比较各种钛合金α”的晶体结构。从这一分析中可以看出,沿b.c.c - cmcm - h.c.p的大部分结构构型。淬火合金中没有观察到相变路径。在理想的Cmcm晶体结构中,确定了未观察到和剩余观察到的构型之间的阈值,相对于实验发现的α”沿着其c轴被压缩。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A general model for the crystal structure of orthorhombic martensite in Ti alloys
The present work develops a novel unified approach to describe the crystal structure of orthorhombic martensite (α′′) in Ti alloys independent of chemical composition. By employing a straightforward yet highly instructive solid sphere model for the basic tetrahedral structural unit the crystal structures involved in the β ↔ α′′/α′ martensitic transformation are categorized into several intermediate configurations. Importantly, a new metric is introduced, δ, which unambiguously characterizes the atomic positions inside the orthorhombic unit cell depending on unit-cell geometry. Furthermore, the exclusive use of relative quantities to describe unit-cell geometry and atom positions renders the approach developed herein independent of alloy content. In this way, shortcomings of commonly suggested structural metrics for α′′ are eliminated. Subsequently, the novel methodology is applied to analyse and compare the crystal structure of α′′ across a broad range of Ti alloys based on experimentally measured unit-cell parameters. From this analysis it emerges that a large fraction of structural configurations along the b.c.c.–Cmcm–h.c.p. transformation path is not observed in quenched alloys. The threshold between the not-observed and the remaining well observed configurations is identified with an ideal Cmcm crystal structure, relative to which the experimentally found α′′ is compressed along its c axis.
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