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原位高温蠕变试验期间SX高温合金通道内的位错密度和速度

Dislocation Densities and Velocities within the Channels of an SX Superalloy during In Situ High-Temperature Creep Tests.

作者信息

Schenk Thomas, Trehorel Roxane, Dirand Laura, Jacques Alain

机构信息

Institute Jean Lamour, CNRS UMR 7198, 54011 Nancy, France.

Laboratory of Excellence on Design of Alloy Metals for low-mAss Structures (DAMAS), Université de Lorraine, 57073 Metz, France.

出版信息

Materials (Basel). 2018 Aug 24;11(9):1527. doi: 10.3390/ma11091527.

DOI:10.3390/ma11091527
PMID:30149568
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6164353/
Abstract

The high-temperature creep behavior of a rafted [001] oriented AM1 Ni-based single crystal superalloy was investigated during in situ creep tests on synchrotrons. Experiments were performed at constant temperatures under variable applied stress in order to study the response (plastic strain, load transfer) to stress jumps. Using two different diffraction techniques in transmission (Laue) geometry, it was possible to measure the average lattice parameters of both the γ matrix and the γ ' rafts in the [100] direction at intervals shorter than 300 s. The absolute precision with both diffraction techniques of the constrained transverse mismatch (in the rafts' plane) is about 10. After stress jumps, special attention is given to the evolution of plastic strain within the γ channels. The relaxation of the Von Mises stress at leveled applied stress shows evidence of dislocation multiplication within the γ channels. From the analysis, we showed an interaction between plastic stress and dislocation density of the γ phase.

摘要

在同步加速器上进行原位蠕变试验期间,研究了筏排[001]取向的AM1镍基单晶高温合金的高温蠕变行为。在恒定温度和可变外加应力下进行实验,以研究对应力突变的响应(塑性应变、载荷传递)。在透射(劳厄)几何构型中使用两种不同的衍射技术,能够以短于300秒的间隔测量[100]方向上γ基体和γ'筏排的平均晶格参数。两种衍射技术对约束横向失配(在筏排平面内)的绝对精度约为10。应力突变后,特别关注γ通道内塑性应变的演变。在恒定外加应力下冯·米塞斯应力的松弛表明γ通道内存在位错增殖。通过分析,我们揭示了塑性应力与γ相的位错密度之间的相互作用。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/216f61bff323/materials-11-01527-g014.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/e37418704452/materials-11-01527-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/7f9c7f1f5fba/materials-11-01527-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/afae66c1ff3c/materials-11-01527-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/396ab8d97615/materials-11-01527-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/216f61bff323/materials-11-01527-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/0180d1e17381/materials-11-01527-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/f11e3864d4c3/materials-11-01527-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/609fb7b5c0ec/materials-11-01527-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/0ec90938b1bb/materials-11-01527-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/df9de3a5dfbf/materials-11-01527-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/02767a260051/materials-11-01527-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/7cfdd6e3fea1/materials-11-01527-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/06d69d56389a/materials-11-01527-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/0e6a734ef3b7/materials-11-01527-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/e37418704452/materials-11-01527-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/7f9c7f1f5fba/materials-11-01527-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/afae66c1ff3c/materials-11-01527-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/396ab8d97615/materials-11-01527-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4bf4/6164353/216f61bff323/materials-11-01527-g014.jpg

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