Measuring the five-parameter grain-boundary distribution from observations of planar sections

被引:223
作者
Saylor, DM [1 ]
El-Dasher, BS
Adams, BL
Rohrer, GS
机构
[1] NIST, Gaithersburg, MD 20899 USA
[2] Lawrence Livermore Natl Lab, Livermore, CA 94550 USA
[3] Brigham Young Univ, Dept Mech Engn, Provo, UT 84602 USA
[4] Carnegie Mellon Univ, Dept Mat Sci & Engn, Pittsburgh, PA 15213 USA
来源
METALLURGICAL AND MATERIALS TRANSACTIONS A-PHYSICAL METALLURGY AND MATERIALS SCIENCE | 2004年 / 35A卷 / 07期
关键词
Material Transaction; Boundary Plane; Plane Normal; Stereological Analysis; Stereological Method;
D O I
10.1007/s11661-004-0147-z
中图分类号
T [工业技术];
学科分类号
08 [工学];
摘要
A stereological method is described for estimating the distribution of grain-boundary types in polycrystalline materials on the basis of observations from a single planar section. The grain-boundary distribution is expressed in terms of five macroscopically observable parameters that include: three parameters that describe the lattice misorientation across the boundary and two parameters that describe the orientation of the grain-boundary plane normal. The grain-boundary distribution is derived from measurements of grain orientations and the orientations of the lines formed where grain boundaries intersect the plane of observation. Tests of the method on simulated observations illustrate that the distribution of boundaries in a material with cubic symmetry can be reliably determined with about 10degrees of resolution from the analysis of 5 X 10degrees or more line segments. Furthermore, grain-boundary distributions directly observed from serial sections of a SrTiO3 polycrystal are compared to those resulting from the stereological analysis of a single plane. The comparison shows that the stereological method provides a reasonable estimate of the measured distribution. The differences between the directly observed grain-boundary distribution and that derived from the stereological analysis are consistent with the results from the simulation.
引用
收藏
页码:1981 / 1989
页数:9
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