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 46
... tetragonal axes are marked a and the third one c , etc. At first glance , the list of Bravais lattices in Table 2-2 appears incomplete . Why not , for example , a base - centered tetragonal lattice ? The full lines in Fig . 2-11 ...
... tetragonal axes are marked a and the third one c , etc. At first glance , the list of Bravais lattices in Table 2-2 appears incomplete . Why not , for example , a base - centered tetragonal lattice ? The full lines in Fig . 2-11 ...
Page 47
... tetragonal cell has only one 4 - fold axis , and this symmetry requires that only two cell edges be equal , namely , the two that are at right angles to the rotation axis . The minimum number of symmetry elements possessed by each ...
... tetragonal cell has only one 4 - fold axis , and this symmetry requires that only two cell edges be equal , namely , the two that are at right angles to the rotation axis . The minimum number of symmetry elements possessed by each ...
Page 323
... tetragonal b ( b ) II - orthorhombic Figure 10-10 Unit cells of the two ordered forms of AuCu . 9 Fig . 10-10 ( b ) , is formed by placing ten tetragonal cells like that of I side by side and then translating five of them by the vectors ...
... tetragonal b ( b ) II - orthorhombic Figure 10-10 Unit cells of the two ordered forms of AuCu . 9 Fig . 10-10 ( b ) , is formed by placing ten tetragonal cells like that of I side by side and then translating five of them by the vectors ...
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