Elements of X-ray DiffractionIntended to acquaint the reader with the theory of x-ray diffraction, the experimental methods involved, and the main applications. The book is a collection of principles and methods stressing X-ray diffraction rather than metallurgy. KEY TOPICS: The book is written entirely in terms of the Bragg law and can be read without any knowledge of the reciprocal lattice. It is divided into three main parts--Fundamentals; experimental methods; and applications. MARKET: Designed for beginners, not as a reference tool for the advanced reader. |
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Page 37
Bernard Dennis Cullity, Stuart R. Stock. Determining the Miller indices of the plane shown in Fig . 2-4 ( b ) requires the following steps . 48 18 88 48 ЗА 3Å Axial lengths Intercept lengths Fractional intercepts Miller indices 1/2 1/4 4 ...
Bernard Dennis Cullity, Stuart R. Stock. Determining the Miller indices of the plane shown in Fig . 2-4 ( b ) requires the following steps . 48 18 88 48 ЗА 3Å Axial lengths Intercept lengths Fractional intercepts Miller indices 1/2 1/4 4 ...
Page 50
... indices of the zone axis . Such planes may have quite different indices and spacings , the only requirement being that they are parallel to a single line . Figure 2-14 shows some examples . If the axis of a zone has indices ( uvw ) ...
... indices of the zone axis . Such planes may have quite different indices and spacings , the only requirement being that they are parallel to a single line . Figure 2-14 shows some examples . If the axis of a zone has indices ( uvw ) ...
Page 52
... indices were devised , namely , to give similar indices to similar planes . For example , the side planes of the hexagonal prism in Fig . 2-15 ( b ) are all similar and symmetrically located , and their relationship is clearly shown in ...
... indices were devised , namely , to give similar indices to similar planes . For example , the side planes of the hexagonal prism in Fig . 2-15 ( b ) are all similar and symmetrically located , and their relationship is clearly shown in ...
Contents
Geometry of Crystals | 31 |
Geometry | 89 |
Intensities Diffraction | 123 |
Copyright | |
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absorption alloy angle appear applied atoms axis calculated called camera cause circle complete consider constant contains counting crystal cubic curve depends described detector determined diffracted beam diffraction lines diffraction pattern diffractometer direction distance effect electrons energy equal equation error example factor Figure film fraction function given grain hexagonal incident beam increases indices intensity kind lattice Laue material means measured metal method normal Note observed obtained occur orientation origin parallel parameter particular pattern peak percent phase plane plot pole position possible powder produce projection radiation rays reciprocal lattice recorded reference reflection region relation relative result rotation sample scattering shown shown in Fig shows simple single solid space specimen sphere stress structure surface temperature tion transmission tube unit cell usually vector wave wavelength x-ray