Elements of X-ray DiffractionThis is a reproduction of a book published before 1923. This book may have occasional imperfections such as missing or blurred pages, poor pictures, errant marks, etc. that were either part of the original artifact, or were introduced by the scanning process. We believe this work is culturally important, and despite the imperfections, have elected to bring it back into print as part of our continuing commitment to the preservation of printed works worldwide. We appreciate your understanding of the imperfections in the preservation process, and hope you enjoy this valuable book. |
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Page 83
Bernard Dennis Cullity. We have here regarded a diffracted beam as being built up of rays scat- tered by successive planes of atoms within the crystal . It would be a mistake to assume , however , that a single plane of atoms A would ...
Bernard Dennis Cullity. We have here regarded a diffracted beam as being built up of rays scat- tered by successive planes of atoms within the crystal . It would be a mistake to assume , however , that a single plane of atoms A would ...
Page 89
... beams to zero . In such a case , there is simply no diffracted beam at the angle predicted by an equation of the type of Eqs . ( 3-10 ) and ( 3–11 ) . It is in this sense that equations of this kind predict all possible diffracted beams ...
... beams to zero . In such a case , there is simply no diffracted beam at the angle predicted by an equation of the type of Eqs . ( 3-10 ) and ( 3–11 ) . It is in this sense that equations of this kind predict all possible diffracted beams ...
Page 289
... diffracted beam . To do this with a fixed counter , the counter slits must be as wide as the diffracted beam for all values of a so that the whole width of the beam can enter the counter . The ideal incident beam for this method is a ...
... diffracted beam . To do this with a fixed counter , the counter slits must be as wide as the diffracted beam for all values of a so that the whole width of the beam can enter the counter . The ideal incident beam for this method is a ...
Contents
THE GEOMETRY OF CRYSTALS | 29 |
CHAPTER 3 | 78 |
CHAPTER 4 | 104 |
Copyright | |
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Common terms and phrases
absorption coefficient absorption edge alloy analysis angle atomic number austenite axis back-reflection Bragg angle Bragg law Bravais lattice calculated camera circle composition constant cos² counter crystal cubic curve Debye ring Debye-Scherrer decrease determined diffracted beam diffraction lines diffraction pattern diffractometer direction distance electrons elements equation error example face-centered face-centered cubic factor film filter fluorescent fluorescent radiation given grain hexagonal incident beam indices integrated intensity lattice parameter martensite measured metal normal obtained orientation Orthorhombic parallel percent phase photograph pinhole pole figure position powder pattern produced projection pulses rays reciprocal lattice reciprocal-lattice reflecting planes relative residual stress rhombohedral rotation sample scattering shown in Fig sin² slit solid solution spacing specimen spectrometer sphere spots stereographic structure substance surface temperature tetragonal thickness tion transmission twin unit cell values vector voltage wave wavelength x-ray diffraction x-ray method x-ray tube zero zone