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
... x - rays . Diffraction and reflection , however , differ fundamentally in at least three aspects : ( 1 ) The diffracted beam from a crystal is built up of rays scattered by all the atoms of the crystal which lie in the path of the incident ...
... x - rays . Diffraction and reflection , however , differ fundamentally in at least three aspects : ( 1 ) The diffracted beam from a crystal is built up of rays scattered by all the atoms of the crystal which lie in the path of the incident ...
Page 105
... x - rays . 4-2 Scattering by an electron . We have seen in Chap . 1 that an x - ray beam is an electromagnetic wave characterized by an electric field whose strength varies sinusoidally with time at any one point in the beam . Since an ...
... x - rays . 4-2 Scattering by an electron . We have seen in Chap . 1 that an x - ray beam is an electromagnetic wave characterized by an electric field whose strength varies sinusoidally with time at any one point in the beam . Since an ...
Page 144
Bernard Dennis Cullity. relative to the x - ray beam . In this case , a three - circle goniometer is used ( Fig . 5-7 ) ... beam . The mechanical stage from a microscope can be easily converted to this purpose . It is often necessary to ...
Bernard Dennis Cullity. relative to the x - ray beam . In this case , a three - circle goniometer is used ( Fig . 5-7 ) ... beam . The mechanical stage from a microscope can be easily converted to this purpose . It is often necessary to ...
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 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