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 84
Page 127
... particular hkl reflec- tion shown , ON is the normal to this set of planes in one particle of the powder . Suppose that the range of angles near the Bragg angle over which reflection is appreciable is 0 . Then , for this particular ...
... particular hkl reflec- tion shown , ON is the normal to this set of planes in one particle of the powder . Suppose that the range of angles near the Bragg angle over which reflection is appreciable is 0 . Then , for this particular ...
Page 225
... particular direction in the crystal . There are alternate ways of manipulating both the Greninger chart and the stereographic projection , and the particular method used is purely a matter of personal preference . For example , we may ...
... particular direction in the crystal . There are alternate ways of manipulating both the Greninger chart and the stereographic projection , and the particular method used is purely a matter of personal preference . For example , we may ...
Page 449
... particular orientation relative to the incident beam , and therefore a particular orien- tation with respect to the measured stress , are able to reflect . There is therefore no good reason why the mechanically measured values of E and ...
... particular orientation relative to the incident beam , and therefore a particular orien- tation with respect to the measured stress , are able to reflect . There is therefore no good reason why the mechanically measured values of E and ...
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