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 315
Bernard Dennis Cullity, Stuart R. Stock. Te Interatomic distance is therefore a / 4 = 2.80 Å . For comparison a “ theoretical ” Cd - Te interatomic distance can be found simply by averaging the distances of closest approach in the pure ...
Bernard Dennis Cullity, Stuart R. Stock. Te Interatomic distance is therefore a / 4 = 2.80 Å . For comparison a “ theoretical ” Cd - Te interatomic distance can be found simply by averaging the distances of closest approach in the pure ...
Page 486
... distance PQ corresponding to each distance OS is then calculated from Eqs . ( 16-4 ) and ( 16-6 ) , and marked off from the center of the ruler in the opposite direction . Corresponding graduations are given the same number and the ...
... distance PQ corresponding to each distance OS is then calculated from Eqs . ( 16-4 ) and ( 16-6 ) , and marked off from the center of the ruler in the opposite direction . Corresponding graduations are given the same number and the ...
Page 587
... distance and has units of inverse length and let is the effective deviation parameter given by left = V ( opf + $ 2 ) ( 20-7 ) a = Note the similarity of Eq . 20-6 to the interference function defined in Eq . 5-8 ; also , the diffracted ...
... distance and has units of inverse length and let is the effective deviation parameter given by left = V ( opf + $ 2 ) ( 20-7 ) a = Note the similarity of Eq . 20-6 to the interference function defined in Eq . 5-8 ; also , the diffracted ...
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