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 1
CHAPTER 1 PROPERTIES OF X - RAYS 1 - 1 Introduction . X - rays were
discovered in 1895 by the German physicist Roentgen and were so named
because their nature was unknown at the time . Unlike ordinary light , these rays
were ...
CHAPTER 1 PROPERTIES OF X - RAYS 1 - 1 Introduction . X - rays were
discovered in 1895 by the German physicist Roentgen and were so named
because their nature was unknown at the time . Unlike ordinary light , these rays
were ...
Page 80
Now consider an imaginary experiment , in which ray 3 is allowed to continue in
a straight line but ray 2 is diverted by some means into a curved path before
rejoining ray 3 . What is the situation on the wave front BB ' where both rays are ...
Now consider an imaginary experiment , in which ray 3 is allowed to continue in
a straight line but ray 2 is diverted by some means into a curved path before
rejoining ray 3 . What is the situation on the wave front BB ' where both rays are ...
Page 82
the path difference for rays 1K1 ' and 2L2 ' is ML + LN = d ' sin 0 + d ' sin 0 . This is
also the path difference for the overlapping rays scattered by S and P in the
direction shown , since in this direction there is no path difference between rays ...
the path difference for rays 1K1 ' and 2L2 ' is ML + LN = d ' sin 0 + d ' sin 0 . This is
also the path difference for the overlapping rays scattered by S and P in the
direction shown , since in this direction there is no path difference between rays ...
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LibraryThing Review
User Review - ron_benson - LibraryThingExcellent reference book. Needs some updating in terms of advances in detector technology. Read full review
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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 angle applied atoms axis back-reflection calculated camera cause chart circle composition consider constant contains continuous copper corresponding 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 means measured metal method normal observed obtained occur orientation parallel parameter particular pattern percent phase photograph plane plotted pole position powder produced projection proportional pulses radiation rays reference reflection relation relative result rotation sample scale scattering shown in Fig shows simple single slit solution spacing specimen stress structure substance surface temperature thickness tion transmission tube twin unit cell usually voltage wave wavelength x-ray zone
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 |
| Original from | University of Minnesota |
| Digitized | 15 Jan 2010 |
| ISBN | 0201012308, 9780201012309 |
| Length | 514 pages |
| Export Citation | BiBTeX EndNote RefMan |