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 12
... caused by electronic transitions within the atom and is best considered from the viewpoint of the quantum theory of radiation . Just as an electron of sufficient energy can knock a K electron , for example , out of an atom and thus cause ...
... caused by electronic transitions within the atom and is best considered from the viewpoint of the quantum theory of radiation . Just as an electron of sufficient energy can knock a K electron , for example , out of an atom and thus cause ...
Page 166
... causes . The two effects together may cause the weakest diffraction line to be almost invisible in relation to the background . This background intensity is due to the following causes : ( 1 ) Fluorescent radiation emitted by the ...
... causes . The two effects together may cause the weakest diffraction line to be almost invisible in relation to the background . This background intensity is due to the following causes : ( 1 ) Fluorescent radiation emitted by the ...
Page 265
... cause of broadening , with grain fragmentation possibly a minor contributing cause . Actually , it is impossible to generalize , inasmuch as different metals and alloys may behave quite differently . By advanced methods of mathematical ...
... cause of broadening , with grain fragmentation possibly a minor contributing cause . Actually , it is impossible to generalize , inasmuch as different metals and alloys may behave quite differently . By advanced methods of mathematical ...
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