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 151
... specimen of no absorption . A calculation of this effect shows that the relative absorption increases as decreases , for any given cylindrical specimen . That this must be so can be seen from Fig . 4-19 ( b ) which applies to a specimen ...
... specimen of no absorption . A calculation of this effect shows that the relative absorption increases as decreases , for any given cylindrical specimen . That this must be so can be seen from Fig . 4-19 ( b ) which applies to a specimen ...
Page 254
... specimen thickness which produces the maximum diffracted intensity is given by 1 / n , where u is the linear absorption coefficient of the specimen . Inspection of Eq . ( 1-10 ) shows that this condition can also be stated as follows ...
... specimen thickness which produces the maximum diffracted intensity is given by 1 / n , where u is the linear absorption coefficient of the specimen . Inspection of Eq . ( 1-10 ) shows that this condition can also be stated as follows ...
Page 417
Bernard Dennis Cullity, Stuart R. Stock. When the specimen is rotated about the axis AA ' , the axis BB'normal to the specimen surface rotates in a vertical plane , but CN , the diffraction plane normal remains fixed in a horizontal ...
Bernard Dennis Cullity, Stuart R. Stock. When the specimen is rotated about the axis AA ' , the axis BB'normal to the specimen surface rotates in a vertical plane , but CN , the diffraction plane normal remains fixed in a horizontal ...
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