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 62
Page 91
... zero . The two rays are therefore out of phase . Adding these two imaginary components of the beam together , produces the form of beam 1 shown in the upper right of the drawing . If the amplitudes of rays 2 and 3 are each 1 unit , then ...
... zero . The two rays are therefore out of phase . Adding these two imaginary components of the beam together , produces the form of beam 1 shown in the upper right of the drawing . If the amplitudes of rays 2 and 3 are each 1 unit , then ...
Page 169
... zero . It follows that the diffracted intensities at angles near 208 , but not greater than 20 , or less than 282 , are not zero but have values intermediate between zero and the maximum intensity of the beam diffracted at an angle 208 ...
... zero . It follows that the diffracted intensities at angles near 208 , but not greater than 20 , or less than 282 , are not zero but have values intermediate between zero and the maximum intensity of the beam diffracted at an angle 208 ...
Page 582
... zero . ( b ) Orientation of the incident beam , the Ewald sphere , g and hkl relrod for deviation parameter less than zero ( left ) , equal to zero ( middle ) and greater than zero ( right ) . - next and the use of higher order Kikuchi ...
... zero . ( b ) Orientation of the incident beam , the Ewald sphere , g and hkl relrod for deviation parameter less than zero ( left ) , equal to zero ( middle ) and greater than zero ( right ) . - next and the use of higher order Kikuchi ...
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