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Quantitative Determination of Preferred Orientation

机译:定量确定首选方向

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摘要

Solutions are presented to the problems which usually prevent accurate x-ray determinations of preferred orientation. The relationship between observed and corrected intensities and the angle dependent absorption factors are treated, including the case of displaced and distorted line profiles caused by low absorption in thick specimens. The absorption factors are derived experimentally from measurements of the scattered (Compton) background radiation without recourse to calculations or tables. Two simple methods, either by varying the wavelength λ or the order n of the x-ray reflection, span the region of the pole figure in which data are unreliable or unobtainable if only one wavelength or order is used. Random samples are not required for normalizing the data to ``times random'''' units. The intensity for a random sample can be calculated from the corrected data itself and the equation Ihkl=[[double integral operator]Ihkl(α,β) sinαdαdβ]/2π where (α,β) are the coordinates of a point on the usual polar net. It is suggested that textures can generally be represented by Gaussian or superposition of Gaussian orientation distributions.
机译:提出了解决这些问题的方法,这些问题通常会妨碍对首选方向的精确X射线确定。处理了观察到的强度和校正后的强度与取决于角度的吸收系数之间的关系,包括由厚样品中的低吸收引起的线轮廓发生位移和变形的情况。吸收系数是从散射(康普顿)背景辐射的测量值通过实验得出的,而无需借助计算或表格。通过改变波长λ或X射线反射的阶数n的两种简单方法,跨越极坐标图的区域,如果仅使用一个波长或阶数,则数据不可靠或无法获得。不需要将数据标准化为``时间随机''单位的随机样本。可以从校正后的数据本身计算出随机样本的强度,方程式Ihkl = [[双积分算子] Ihkl(α,β)sinαdαdβ] /2π其中,(α,β)是通常点的坐标极网。建议纹理通常可以用高斯或高斯方向分布的叠加表示。

著录项

  • 来源
    《Journal of Applied Physics》 |1964年第4期|共7页
  • 作者单位

    Materials Sciences Laboratory, Lockheed Missiles and Space Company, Palo Alto, California;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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