Relationship between the superelasticity and strain field around Ni4Ti3 nano-precipitates in NiTi shape memory alloy via laser powder bed fusion

IF 6.1 1区 工程技术 Q1 ENGINEERING, MANUFACTURING
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Abstract

Although the simulation results had demonstrated that the strain field introduced by Ni4Ti3 nano-precipitates in NiTi shape memory alloys (SMAs) was related with their superelasticity inherently, the corresponding experimental result was rarely documented heretofore, especially in additive manufactured NiTi SMAs. In this work, we tailor the morphologies and resultant strain field of Ni4Ti3 nano-precipitates by heat treatment of a NiTi SMA subjected to laser powder bed fusion (LPBF), and further authenticate relationship between the superelasticity and the strain field in the LPBF NiTi samples. When holding times were 1 h, 3 h, and 5 h at aging temperature of 350 °C after solution treatment, the Ni4Ti3 nano-precipitates in the LPBF NiTi samples exhibit spherical, ellipsoidal, and lenticular morphologies, respectively. Accordingly, the strain field around Ni4Ti3 nano-precipitates in B2 matrix decrease from 0.15 % to 0.13 % and 0.10 %, respectively. The LPBF and aged NiTi samples present large superelasticity, which exceeds 6 % recovery strain together with high recovery rate of ˃99 % during 10-times cyclic compression loading. Interestingly, the LPBF and aged sample with the spherical Ni4Ti3 and highest strain field displays the worst superelasticity stability, while the one with the lenticular Ni4Ti3 and smallest strain field exhibits the relatively stable and biggest superelasticity of 6.36 %. Basically, this is attributed to different mechanisms between the Ni4Ti3 nano-precipitates and dislocations generated during cyclic loading, which is induced by different interfaces between the Ni4Ti3 and B2 matrix in the three types of the NiTi samples. For the sample with the highest strain field, its spherical Ni4Ti3 was cut through by generated dislocations due to coherent interface between the spherical Ni4Ti3 and B2 matrix. In contrast, the one with the smallest strain field, its lenticular Ni4Ti3 can impede effectively generated dislocations because of semi-coherent or non-coherent interface between the lenticular Ni4Ti3 and B2 matrix. Therefore, these results can provide meaningful insights into tailoring the nano-precipitates and thereby obtaining excellent superelasticity of NiTi SMAs by LPBF.

Abstract Image

通过激光粉末床熔融技术获得镍钛形状记忆合金中 Ni4Ti3 纳米沉淀物周围的超弹性和应变场之间的关系
尽管模拟结果表明,Ni4Ti3 纳米沉淀物在镍钛形状记忆合金(SMA)中引入的应变场与其固有的超弹性有关,但相应的实验结果迄今为止却鲜有记录,尤其是在添加剂制造的镍钛 SMA 中。在这项工作中,我们通过对经过激光粉末床熔融(LPBF)的镍钛 SMA 进行热处理,定制了镍钛 3 纳米沉淀物的形态和应变场,并进一步验证了 LPBF 镍钛样品的超弹性和应变场之间的关系。当溶液处理后在 350 ℃ 的老化温度下保持 1 小时、3 小时和 5 小时时,LPBF NiTi 样品中的 Ni4Ti3 纳米沉淀物分别呈现球形、椭圆形和透镜状。因此,B2 基体中 Ni4Ti3 纳米沉淀周围的应变场分别从 0.15 % 下降到 0.13 % 和 0.10 %。LPBF 和老化镍钛样品具有很大的超弹性,在 10 次循环压缩加载过程中,恢复应变超过 6%,恢复率高达 ˃99 %。有趣的是,球形 Ni4Ti3 和最大应变场的 LPBF 和老化样品显示出最差的超弹性稳定性,而透镜状 Ni4Ti3 和最小应变场的样品显示出相对稳定和最大的超弹性,达到 6.36 %。这主要归因于三种镍钛样品中镍钛三纳米沉淀物和位错在循环加载过程中产生的机制不同,而镍钛三纳米沉淀物和 B2 基体之间的界面也不同。应变场最大的样品中,由于球形 Ni4Ti3 和 B2 基体之间的相干界面产生了位错,球形 Ni4Ti3 被位错切割。相反,应变场最小的样品,其透镜状的 Ni4Ti3 由于透镜状 Ni4Ti3 和 B2 基体之间的半相干或非相干界面,能有效地阻碍位错的产生。因此,这些结果可为定制纳米沉淀物,从而通过 LPBF 获得优异的镍钛 SMA 超弹性提供有意义的启示。
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来源期刊
Journal of Manufacturing Processes
Journal of Manufacturing Processes ENGINEERING, MANUFACTURING-
CiteScore
10.20
自引率
11.30%
发文量
833
审稿时长
50 days
期刊介绍: The aim of the Journal of Manufacturing Processes (JMP) is to exchange current and future directions of manufacturing processes research, development and implementation, and to publish archival scholarly literature with a view to advancing state-of-the-art manufacturing processes and encouraging innovation for developing new and efficient processes. The journal will also publish from other research communities for rapid communication of innovative new concepts. Special-topic issues on emerging technologies and invited papers will also be published.
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