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 94
... x - ray beam is extremely small compared to that of the incident beam . Despite these differences , the terms “ reflecting planes ” and “ reflected beams ” are often used when diffracting planes and diffracted beams are described . This ...
... x - ray beam is extremely small compared to that of the incident beam . Despite these differences , the terms “ reflecting planes ” and “ reflected beams ” are often used when diffracting planes and diffracted beams are described . This ...
Page 124
... beam is changed , not necessarily to zero , by any change in atomic ... x - rays are scattered by a single electron , then by an atom , and finally by all the atoms in the unit cell . These results are applied next to the powder method of x - ...
... beam is changed , not necessarily to zero , by any change in atomic ... x - rays are scattered by a single electron , then by an atom , and finally by all the atoms in the unit cell . These results are applied next to the powder method of x - ...
Page 126
... beam whose intensity at P is found from Eq . ( 4-1 ) to be K Ipy = loy 2 since a = 4yOP = 7/2 . Similarly , the ... x - ray beam by a single electron . The intensity of the scattered beam is only a minute fraction of the intensity of the ...
... beam whose intensity at P is found from Eq . ( 4-1 ) to be K Ipy = loy 2 since a = 4yOP = 7/2 . Similarly , the ... x - ray beam by a single electron . The intensity of the scattered beam is only a minute fraction of the intensity 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