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. |
From inside the book
Results 1-3 of 47
Page 35
... origin of the lattice lies on a lattice point and if u ' , v ' and w ' are integers , the point located by r must be ... origin parallel to the given line and then giving the coordinates of any point on the line through the origin . Let ...
... origin of the lattice lies on a lattice point and if u ' , v ' and w ' are integers , the point located by r must be ... origin parallel to the given line and then giving the coordinates of any point on the line through the origin . Let ...
Page 48
... origin of the unit cell to the given point has components xa , yb , zc , where x , y , and z are fractions , then the coordinates of the point are x y z . Thus , point A in Fig . 2-13 , taken as the origin , has coordinates 0 0 0 while ...
... origin of the unit cell to the given point has components xa , yb , zc , where x , y , and z are fractions , then the coordinates of the point are x y z . Thus , point A in Fig . 2-13 , taken as the origin , has coordinates 0 0 0 while ...
Page 109
... origin of the reciprocal lattice , and each has a different origin ( Fig . 3-13 ) . Thus , each incident beam S / 1 ; has a corresponding Ewald sphere touching the origin of the reciprocal lattice and having radius 1/4 ;. All of the ...
... origin of the reciprocal lattice , and each has a different origin ( Fig . 3-13 ) . Thus , each incident beam S / 1 ; has a corresponding Ewald sphere touching the origin of the reciprocal lattice and having radius 1/4 ;. All of the ...
Contents
Geometry of Crystals | 31 |
Geometry | 89 |
Intensities Diffraction | 123 |
Copyright | |
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Common terms and phrases
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