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
An accelerated electric charge radiates energy. The acceleration may, of course,
be either positive or negative, and thus a charge continuously oscillating about
some mean position acts as an excellent source of electromagnetic radiation.
An accelerated electric charge radiates energy. The acceleration may, of course,
be either positive or negative, and thus a charge continuously oscillating about
some mean position acts as an excellent source of electromagnetic radiation.
Page 12
It takes place in all directions, and since the energy in the scattered beams does
not appear in the transmitted beam, it is, so far as the transmitted beam is
concerned, said to be absorbed. The phenomenon of scattering will be discussed
in ...
It takes place in all directions, and since the energy in the scattered beams does
not appear in the transmitted beam, it is, so far as the transmitted beam is
concerned, said to be absorbed. The phenomenon of scattering will be discussed
in ...
Page 13
True absorption is now occurring and a large fraction of the incident quanta
simply disappear, their energy being converted into fluorescent radiation and the
kinetic energy of ejected photoelectrons. Since energy must be conserved in the
...
True absorption is now occurring and a large fraction of the incident quanta
simply disappear, their energy being converted into fluorescent radiation and the
kinetic energy of ejected photoelectrons. Since energy must be conserved in the
...
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User Review - ron_benson - LibraryThingExcellent reference book. Needs some updating in terms of advances in detector technology. Read full review
Contents
PROPERTIES OF XRAYs | 1 |
THE GEOMETRY OF CRYSTALs | 29 |
THE DIRECTIONs of DIFFRACTED BEAMs | 78 |
Copyright | |
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Elements of X-ray Diffraction Bernard Dennis Cullity,Stuart R. Stock,Stuart R.. Stock Snippet view - 2001 |
Common terms and phrases
absorption alloy analysis angle applied atoms axis Bragg calculated camera cause circle composition consider constant contains continuous copper counter counting crystal cubic curve decreases depends described determined diffracted beam diffraction lines diffractometer direction distance effect electrons elements energy equal equation error example factor Figure film fluorescent given gives grain hexagonal incident beam increases indices intensity involved kind known lattice Laue length located material means measured metal method normal observed obtained occur orientation parallel parameter particular pattern percent phase photograph plane plotted pole position possible powder produced projection proportional pulses radiation rays reference reflection relation relative result rotation sample scattering shown shown in Fig shows simple single solid solution spacing specimen stress structure substance surface temperature thickness tion tube twin unit cell usually vector voltage wave wavelength x-ray
Bibliographic information
| Title | Elements of X-ray Diffraction Volume 5 of Addison-Wesley metallurgy series Volume 1230 of Addison-Wesley series in metallurgy and materials |
| Author | Bernard Dennis Cullity |
| Edition | 3 |
| Publisher | Addison-Wesley Publishing Company, 1956 |
| ISBN | 0201012308, 9780201012309 |
| Length | 514 pages |
| Export Citation | BiBTeX EndNote RefMan |