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 267
... region , as shown in Fig . 3-10 ( a ) and ( b ) ; it is in this region also that the temperature - diffuse scattering is most intense . In both Laue methods , the short - wavelength radiation in the incident beam will cause most ...
... region , as shown in Fig . 3-10 ( a ) and ( b ) ; it is in this region also that the temperature - diffuse scattering is most intense . In both Laue methods , the short - wavelength radiation in the incident beam will cause most ...
Page 532
... regions have a common direction ( 110 ) , and region 2 ( right of Fig . 17-24 ) is rotated by ยข from region 1. The beam incident on both parts of the crystal is along Sm , the proper direction for 004 diffraction , and , with d2 > dj ...
... regions have a common direction ( 110 ) , and region 2 ( right of Fig . 17-24 ) is rotated by ยข from region 1. The beam incident on both parts of the crystal is along Sm , the proper direction for 004 diffraction , and , with d2 > dj ...
Page 559
... REGION Equation 19-5 expresses scattering from a single particle as a function of the scattering vector J , and , in the small angle region , the exponential function can be expanded as a power series in J , and terms of order higher ...
... REGION Equation 19-5 expresses scattering from a single particle as a function of the scattering vector J , and , in the small angle region , the exponential function can be expanded as a power series in J , and terms of order higher ...
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