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 160
... cos2 20 Line F2 р sin ? 0 cos Calc . Calc . Obs . VS S S S 1 2 3 4 5 6 7 8 7810 6990 4520 3500 3230 2500 2120 1970 8 6 12 24 8 6 24 24 12.03 8.50 3.70 2.83 2.74 3.18 4.81 6.15 7.52 x 105 3.56 2.01 2.38 0.71 0.48 2.45 2.91 10.0 4.7 2.7 ...
... cos2 20 Line F2 р sin ? 0 cos Calc . Calc . Obs . VS S S S 1 2 3 4 5 6 7 8 7810 6990 4520 3500 3230 2500 2120 1970 8 6 12 24 8 6 24 24 12.03 8.50 3.70 2.83 2.74 3.18 4.81 6.15 7.52 x 105 3.56 2.01 2.38 0.71 0.48 2.45 2.91 10.0 4.7 2.7 ...
Page 557
... cos2 20 Fp > exp ( -2M ) ( 4-21 ) sin ? 0 cos o les Figure 19-2 Low angle x - ray diffraction pattern of turkey leg collagen recorded on an image plate . ( Courtesy of Snigirev et al ( 19-3 ] . ) = where I = relative integrated ...
... cos2 20 Fp > exp ( -2M ) ( 4-21 ) sin ? 0 cos o les Figure 19-2 Low angle x - ray diffraction pattern of turkey leg collagen recorded on an image plate . ( Courtesy of Snigirev et al ( 19-3 ] . ) = where I = relative integrated ...
Page 637
... cos2 20. Triclinic : hkl 2 Note that , in cubic crystals , for example , hhl stands for such indices as 112 ( or 211 ) , Okl for such indices as 012 ( or 210 ) , Okk for such indices as 011 ( or 110 ) , etc. These are the usual ...
... cos2 20. Triclinic : hkl 2 Note that , in cubic crystals , for example , hhl stands for such indices as 112 ( or 211 ) , Okl for such indices as 012 ( or 210 ) , Okk for such indices as 011 ( or 110 ) , etc. These are the usual ...
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