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 44
Bernard Dennis Cullity, Stuart R. Stock. TABLE 2.2 CRYSTAL SYSTEMS AND BRAVAIS LATTICES ( The symbol # means that equity is not required by symmetry . Accidental equality may occur , as shown by an example in Sec . 2-4 . ) System Axial ...
Bernard Dennis Cullity, Stuart R. Stock. TABLE 2.2 CRYSTAL SYSTEMS AND BRAVAIS LATTICES ( The symbol # means that equity is not required by symmetry . Accidental equality may occur , as shown by an example in Sec . 2-4 . ) System Axial ...
Page 58
... Bravais lattice , since that is the basic framework on which the crystal is built and because , as Chap . 4 demonstrates , it has a profound effect on the way in which that crystal diffracts x - rays . What is the Bravais lattice of ...
... Bravais lattice , since that is the basic framework on which the crystal is built and because , as Chap . 4 demonstrates , it has a profound effect on the way in which that crystal diffracts x - rays . What is the Bravais lattice of ...
Page 60
... Bravais lattice of the ferrites is face - centered cubic , and the unit cell contains 8 “ molecules ” or a total of 8 x 7 = 56 ions . There are therefore 56/4 or 14 ions associated with each lattice point . The number of atoms per unit ...
... Bravais lattice of the ferrites is face - centered cubic , and the unit cell contains 8 “ molecules ” or a total of 8 x 7 = 56 ions . There are therefore 56/4 or 14 ions associated with each lattice point . The number of atoms per unit ...
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