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 333
... solid solutions a and ß are called primary solid solutions or terminal solid solutions . Or the second phase which appears may have no connection with the B - rich solid solution , as in the system shown in Fig . 11-2 ( b ) . Here the ...
... solid solutions a and ß are called primary solid solutions or terminal solid solutions . Or the second phase which appears may have no connection with the B - rich solid solution , as in the system shown in Fig . 11-2 ( b ) . Here the ...
Page 338
... solid solution of carbon in face - centered cubic y - iron , the addition of carbon increases the cell edge a . But in martensite , a metastable interstitial solid solution of carbon in a - iron , the c parameter of the body - centered ...
... solid solution of carbon in face - centered cubic y - iron , the addition of carbon increases the cell edge a . But in martensite , a metastable interstitial solid solution of carbon in a - iron , the c parameter of the body - centered ...
Page 340
Bernard Dennis Cullity, Stuart R. Stock. Defect substitutional solid solutions are ones in which some lattice sites ... solution in the nickel - aluminum system ( p . 387 , G.8 ) . A defect solution is disclosed by anomalies in the curves ...
Bernard Dennis Cullity, Stuart R. Stock. Defect substitutional solid solutions are ones in which some lattice sites ... solution in the nickel - aluminum system ( p . 387 , G.8 ) . A defect solution is disclosed by anomalies in the curves ...
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