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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Results 1-3 of 81
Page 76
... Fig . 2-29 showed that this angle could be measured on the surface of the sphere along the great circle connecting ... shown in perspective in Fig . 2-29 , and the angle between them is found by the rotation illustrated in Fig . 2-34 ( b ) ...
... Fig . 2-29 showed that this angle could be measured on the surface of the sphere along the great circle connecting ... shown in perspective in Fig . 2-29 , and the angle between them is found by the rotation illustrated in Fig . 2-34 ( b ) ...
Page 100
... shown in Fig . 3-6 for a simple orthorhombic crystal with lattice parameters a , = 2.0 Å , az = 1.0 Å and az = 3.0 Å . The corresponding magnitudes of the reciprocal lattice vectors are bı 0.5 Å ?, b2 = 1.0 Å and bz = 0.33 Å ' , and Fig ...
... shown in Fig . 3-6 for a simple orthorhombic crystal with lattice parameters a , = 2.0 Å , az = 1.0 Å and az = 3.0 Å . The corresponding magnitudes of the reciprocal lattice vectors are bı 0.5 Å ?, b2 = 1.0 Å and bz = 0.33 Å ' , and Fig ...
Page 271
... illustrated in Fig . 8-9 are achieved when the pinholes are about one - third the size of the projected source . If the value of h is smaller than that given by Eq . ( 8-7 ) , then conditions will be intermediate between those shown in Figs ...
... illustrated in Fig . 8-9 are achieved when the pinholes are about one - third the size of the projected source . If the value of h is smaller than that given by Eq . ( 8-7 ) , then conditions will be intermediate between those shown in Figs ...
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