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 404
... texture , but copper , also FCC , a has a double [ 111 ] + [ 100 ] texture ; i.e. , in drawn copper wire there are two sets of grains , the fiber axis of one set being [ 111 ] and that of the other set ( 100 ) . Sheet Texture > In its ...
... texture , but copper , also FCC , a has a double [ 111 ] + [ 100 ] texture ; i.e. , in drawn copper wire there are two sets of grains , the fiber axis of one set being [ 111 ] and that of the other set ( 100 ) . Sheet Texture > In its ...
Page 407
... texture is such that there are very few such grains , the intensity of the hkl reflection will be abnormally low . In another case , a given reflection may have abnormally high intensity , which would indicate that the corresponding ...
... texture is such that there are very few such grains , the intensity of the hkl reflection will be abnormally low . In another case , a given reflection may have abnormally high intensity , which would indicate that the corresponding ...
Page 426
... texture , provided the texture is sharp enough to produce well resolved peaks in the high - d region . This is a fortunate circumstance , because higho measurements require little or no specimen preparation . Preferred orientation in ...
... texture , provided the texture is sharp enough to produce well resolved peaks in the high - d region . This is a fortunate circumstance , because higho measurements require little or no specimen preparation . Preferred orientation in ...
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