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 124
... reflection can occur from their ( 100 ) planes . Other crystals of different orientation may be in such a position that reflection can occur from their ( 010 ) or ( 001 ) planes . Since all these planes have the same spacing , the beams ...
... reflection can occur from their ( 100 ) planes . Other crystals of different orientation may be in such a position that reflection can occur from their ( 010 ) or ( 001 ) planes . Since all these planes have the same spacing , the beams ...
Page 293
... reflecting power , this reflection may be so strong that it may be taken for an h1kil reflection of the Ka wavelength . Apparently the only sure way of eliminating this possibility is to use balanced filters . ( 2 ) The crystal ...
... reflecting power , this reflection may be so strong that it may be taken for an h1kil reflection of the Ka wavelength . Apparently the only sure way of eliminating this possibility is to use balanced filters . ( 2 ) The crystal ...
Page 502
... reflection 410 reflection 120 S S λ 20 410 20 So b1 A CD B AK edge Ag ASWL FIG . A15-12 . Reciprocal - lattice treatment of the Laue method . ( S - So ) / \ = H. To these two extreme wavelengths correspond two extreme reflection spheres ...
... reflection 410 reflection 120 S S λ 20 410 20 So b1 A CD B AK edge Ag ASWL FIG . A15-12 . Reciprocal - lattice treatment of the Laue method . ( S - So ) / \ = H. To these two extreme wavelengths correspond two extreme reflection spheres ...
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 cosē 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 sinē 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