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Grain Boundary Character Distributions In Isostructural Materials.

机译:等构材料中的晶界特征分布。

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摘要

Anisotropic grain boundary character distributions (GBCDs), which influence macroscopic materials properties, are thought to be controlled by the grain boundary energy anisotropy. Structurally, grain boundary could be viewed as two free surfaces joined together. Grain boundary energy could be simply defined by the total excess energy for creating two free surfaces minus the energy gained when new bonds are formed between these surfaces. This implies that different crystal structure should have different GBEDs and GBCDs. It was recently discovered that grain boundary energy distributions (GBED) in isostructural materials, a class of materials that share the same crystal structure, are directly related to one another. This suggests that GBCDs in isostructural materials might also be related in a similar way. To test this hypothesis, electron backscatter diffraction (EBSD) was used to map grain orientations in Ag, Au, Cu, Fe, and Mo. The GBCDs were determined from the stereological interpretation of EBSD maps containing on the order of 100,000 grains. It was found that the GBCDs of face-centered cubic (FCC) metals are statistically correlated, while the GBCDs of body-centered cubic (BCC) Fe and Mo are not correlated to the GBCD of FCC metals. The degree of the correlations among the FCC metals is weaker if there are significant differences in grain shape or texture. For example, Ag has the weakest correlation to the other FCC materials and also has quantitatively different grain shapes and texture. The relationship between the populations and energies of grain boundaries was also studied. By comparing the GBCDs of Al, Au, Cu, and Ni to the energies of 388 grain boundaries previously calculated by the Embedded Atom Method (EAM), we observed a moderately inverse correlation between the relative areas of grain boundaries and their energies. Interestingly, there are strong inverse correlations between the energies and populations of the most common grain boundaries (Sigma3, Sigma9, and Sigma27). Because the enhancement of twin related boundaries due to the prevalence Sigma3 boundaries results in a decrease in the grain boundary populations for the other boundary types, this inverse correlation is influenced by the crystallographic constraints at triple junctions. In other words, having an anisotropic misorientation distribution with strong maxima for certain boundaries biases the inverse correlation between grain boundary population and energy for other boundaries and causes different slopes at each misorientation. Interestingly, the inverse correlation at each misorientation is consistent with the Boltzmann distribution. Based on our results, it is possible to predict the GBCDs and GBEDs in isostructural polycrystalline materials by using a single GBCD and GBED. This principle is demonstrated by predicting the GBCD and GBED of Actinium (Ac).;In this thesis, the results demonstrated that the GBCDs of isostructural materials are correlated with one another and the magnitudes of correlation coefficients varied. Reduced correlations were observed when there were differences in the microstructure and crystallographic texture. The inverse relationship between grain boundary population and energy is more strongly correlated at each misorientation than over the entire five macroscopic parameters of grain boundary, especially when there is significant misorientation texture. This relationship leads to GBCDs of isostructural materials that are also more strongly correlated at each misorientation than over the entire grain boundary space.;To investigate the GBED in the isostructural BCC metals, the energies of 408 grain boundaries in Fe and Mo were computed using atomistic simulations based on the embedded-atom method (EAM) potential. We found that the calculated boundary energies in Fe and Mo were strongly correlated and scaled with the ratio of the cohesive energy divided by the square of the lattice constant (Ecoh/a02). We would expect that the GBCD of Fe and Mo might be correlated in a similar manner to that of FCC metals. To test this hypothesis, we compared the GBCDs of Fe and Mo. We found that the GBCDs of Fe and Mo are moderately and strongly correlated when all boundary types and only Sigma3 boundaries were considered, respectively.
机译:各向异性晶界特征分布(GBCD)影响宏观材料的性能,被认为是受晶界能各向异性控制的。从结构上讲,晶界可以看作是两个自由表面连接在一起。晶界能可以简单地由产生两个自由表面的总多余能量减去在这些表面之间形成新的键合时获得的能量来定义。这意味着不同的晶体结构应具有不同的GBED和GBCD。最近发现,同构材料是一类具有相同晶体结构的材料,其晶界能分布(GBED)与彼此直接相关。这表明同构材料中的GBCD也可能以相似的方式关联。为了验证该假设,使用电子反向散射衍射(EBSD)绘制了Ag,Au,Cu,Fe和Mo中晶粒的方向图。GBCD是根据EBSD图的立体解释确定的,该图包含大约100,000个晶粒。发现面心立方(FCC)金属的GBCD与统计相关,而体心立方(BCC)Fe和Mo的GBCD与FCC金属的GBCD不相关。如果晶粒形状或织构存在显着差异,则FCC金属之间的相关程度较弱。例如,Ag与其他FCC材料的相关性最弱,并且在数量上也具有不同的晶粒形状和质地。还研究了晶界的能量与种群之间的关系。通过将Al,Au,Cu和Ni的GBCD与先前通过嵌入式原子方法(EAM)计算的388个晶界的能量进行比较,我们观察到晶界相对面积与其能之间的适度反相关。有趣的是,在最常见的晶界(Sigma3,Sigma9和Sigma27)的能量和总体之间存在很强的逆相关性。由于存在较高的Sigma3边界,导致孪晶相关边界的增强导致其他边界类型的晶界总体减少,因此这种反向相关性受到三重结处的晶体学约束的影响。换句话说,对于某些边界而言,各向异性取向差分布具有极大的最大值,这会扭曲晶粒边界总体与其他边界的能量之间的反相关关系,并在每个取向差处产生不同的斜率。有趣的是,每个取向错误的逆相关性与玻耳兹曼分布一致。根据我们的结果,可以通过使用单个GBCD和GBED来预测同构多晶材料中的GBCD和GBED。通过预测Act(Ac)的GBCD和GBED证明了这一原理。本论文的结果表明,同构材料的GBCD相互关联,并且相关系数的大小不同。当微观结构和晶体织构存在差异时,相关性降低。与每个晶界的整个五个宏观参数相比,在每种取向方向上,晶界总数与能量之间的反比关系更紧密相关,尤其是当存在明显的取向错误纹理时。这种关系导致同构材料的GBCD与每个晶向相比在整个晶界空间上的相关性也更强。;为了研究同构BCC金属中的GBED,使用原子能计算了Fe和Mo中408晶界的能基于嵌入式原子方法(EAM)势的模拟。我们发现,计算出的Fe和Mo中的边界能与内聚能之比除以晶格常数的平方(Ecoh / a02)高度相关并成比例。我们预计,铁和钼的GBCD可能以与FCC金属相似的方式关联。为了检验该假设,我们比较了Fe和Mo的GBCD。我们发现,当分别考虑所有边界类型和仅Sigma3边界时,Fe和Mo的GBCD呈中等和强相关。

著录项

  • 作者

    Ratanaphan, Sutatch.;

  • 作者单位

    Carnegie Mellon University.;

  • 授予单位 Carnegie Mellon University.;
  • 学科 Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 2013
  • 页码 200 p.
  • 总页数 200
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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