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 322
... AuCu , and the structure of ordered AuCu must therefore be such that the ratio of gold sites to copper sites is also 1 : 1 . Two ordered forms are produced , depending on the ordering temperature , and these have different crystal ...
... AuCu , and the structure of ordered AuCu must therefore be such that the ratio of gold sites to copper sites is also 1 : 1 . Two ordered forms are produced , depending on the ordering temperature , and these have different crystal ...
Page 323
... AuCu . 9 Fig . 10-10 ( b ) , is formed by placing ten tetragonal cells like that of I side by side and then ... AuCu , on the other . In AuCuz there is a change in Bravais lattice , but no change in crystal system , accompanying the ...
... AuCu . 9 Fig . 10-10 ( b ) , is formed by placing ten tetragonal cells like that of I side by side and then ... AuCu , on the other . In AuCuz there is a change in Bravais lattice , but no change in crystal system , accompanying the ...
Page 329
... AuCu , quenched from a temperature T. The ratio of the integrated intensity of the 420 line to that of the 421 line is found to be 4.38 . Calculate the value of the long - range order parameter S at temperature T. ( Take the lattice ...
... AuCu , quenched from a temperature T. The ratio of the integrated intensity of the 420 line to that of the 421 line is found to be 4.38 . Calculate the value of the long - range order parameter S at temperature T. ( Take the lattice ...
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