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 284
... Completing the steps listed above is sufficient for most analyses . For a complete analysis , however , the following should be done . 5. Prepare mixtures of the identified components until the original 284 Phase Identification by X ...
... Completing the steps listed above is sufficient for most analyses . For a complete analysis , however , the following should be done . 5. Prepare mixtures of the identified components until the original 284 Phase Identification by X ...
Page 316
... complete , the probability that a particular site is occupied by a gold atom is simply à , the atomic fraction of gold in the alloy , and the probability that it is occupied by a copper atom is À , the atomic fraction of copper . These ...
... complete , the probability that a particular site is occupied by a gold atom is simply à , the atomic fraction of gold in the alloy , and the probability that it is occupied by a copper atom is À , the atomic fraction of copper . These ...
Page 317
... Complete order . Each unit cell now contains one gold atom , at 000 , and three copper atoms , at ļ , 2,0 , 1 , 0 , į and 0 , 1 , Ż . , 1 1 2 , 2 F = fau + fcule * ish + k ) + ewish + leti ( k + 1 ] ; F = ( fau + 3fcu ) , for hkl ...
... Complete order . Each unit cell now contains one gold atom , at 000 , and three copper atoms , at ļ , 2,0 , 1 , 0 , į and 0 , 1 , Ż . , 1 1 2 , 2 F = fau + fcule * ish + k ) + ewish + leti ( k + 1 ] ; F = ( fau + 3fcu ) , for hkl ...
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