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. |
From inside the book
Results 1-3 of 92
Page 94
... beam formed . If this plane is now rotated about the incident beam as axis in such a way that @ is kept constant , then the reflected beam will travel over the surface of a cone as shown in Fig . 3-11 ( b ) , the axis of the cone ...
... beam formed . If this plane is now rotated about the incident beam as axis in such a way that @ is kept constant , then the reflected beam will travel over the surface of a cone as shown in Fig . 3-11 ( b ) , the axis of the cone ...
Page 106
... incident beam is traveling in the direc- tion Ox ( Fig . 4-3 ) and encounters an electron at O. We wish to know the scattered intensity at P in the xz plane where OP is inclined at a scattering angle of 20 to the incident beam . An ...
... incident beam is traveling in the direc- tion Ox ( Fig . 4-3 ) and encounters an electron at O. We wish to know the scattered intensity at P in the xz plane where OP is inclined at a scattering angle of 20 to the incident beam . An ...
Page 107
... beam is only a minute fraction of the intensity of the incident beam . The equa- tion also shows that the scattered intensity decreases as the inverse square of the distance from the scattering electron , as one would expect , and that ...
... beam is only a minute fraction of the intensity of the incident beam . The equa- tion also shows that the scattered intensity decreases as the inverse square of the distance from the scattering electron , as one would expect , and that ...
Contents
THE GEOMETRY OF CRYSTALS | 29 |
CHAPTER 3 | 78 |
CHAPTER 4 | 104 |
Copyright | |
24 other sections not shown
Other editions - View all
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 cosĀ² 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 sinĀ² 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