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 4
... produced by the oscil- lation of charge back and forth in the broadcasting antenna , and visible light by ... produced when any electri- cally charged particle of sufficient kinetic energy is rapidly decelerated . Electrons are usually ...
... produced by the oscil- lation of charge back and forth in the broadcasting antenna , and visible light by ... produced when any electri- cally charged particle of sufficient kinetic energy is rapidly decelerated . Electrons are usually ...
Page 94
... produced by various metal powders , are shown in Fig . 3-13 . Each diffrac- tion line is made up of a large number ... produced the line . = Conversely , if the shape and size of the unit cell of the crystal are known , we can predict ...
... produced by various metal powders , are shown in Fig . 3-13 . Each diffrac- tion line is made up of a large number ... produced the line . = Conversely , if the shape and size of the unit cell of the crystal are known , we can predict ...
Page 412
... produced by the mosaic structure of the analyzing crystal : this divergence is related to the extent of disorientation of the mosaic blocks , and has a value of about 0.2 ° for the crystals normally used . The line width B is the sum of ...
... produced by the mosaic structure of the analyzing crystal : this divergence is related to the extent of disorientation of the mosaic blocks , and has a value of about 0.2 ° for the crystals normally used . The line width B is the sum of ...
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