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. 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. Designed for beginners, not as a reference tool for the advanced reader. |
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Page 239
... pole , as before , but that PA and P are { 110 } poles . P must then be a { 100 } pole and 6 ' a { 110 ) pole . We can check this assumption by measuring the angles in the triangle ab - 5 ' . Both a and b are found to be 55 ° from 5 ...
... pole , as before , but that PA and P are { 110 } poles . P must then be a { 100 } pole and 6 ' a { 110 ) pole . We can check this assumption by measuring the angles in the triangle ab - 5 ' . Both a and b are found to be 55 ° from 5 ...
Page 313
... pole figure . This texture can therefore be represented by the ideal orientation { 110 } < T12 ) . But the pole figure itself must be regarded as a far better description of the texture than any bare statement of an ideal orientation ...
... pole figure . This texture can therefore be represented by the ideal orientation { 110 } < T12 ) . But the pole figure itself must be regarded as a far better description of the texture than any bare statement of an ideal orientation ...
Page 319
... pole density curve is not necessary for the evaluation of a texture , provided the texture is sharp enough to produce well resolved peaks in the high - ø region . This is a fortunate circumstance ... pole figures Inverse pole figures 300 303.
... pole density curve is not necessary for the evaluation of a texture , provided the texture is sharp enough to produce well resolved peaks in the high - ø region . This is a fortunate circumstance ... pole figures Inverse pole figures 300 303.
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Common terms and phrases
absorption alloy angle applied arrangement atoms axes axis calculated called camera cause circle consider constant contains corresponding counter counting crystal cubic curve depends described determined diffracted beam diffraction lines diffractometer direction distance effect electron elements energy equal equation error example factor figure film given grain hexagonal incident beam increases indices intensity involved kind lattice Laue less located material means measured metal method normal Note observed obtained occur orientation origin parallel parameter particular pattern percent phase photographic plane pole position possible powder produced projection radiation rays reciprocal reference reflection region relation relative result rotation sample scattering sheet shown shown in Fig shows simple single solid solution spacing specimen sphere standard stress structure surface temperature texture transmission tube twin unit cell usually various vector voltage wave wavelength x-ray zone