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. |
From inside the book
Results 1-3 of 92
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 invisible, ...
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 invisible, ...
Page 25
Ionization devices measure the intensity of x-ray beams by the amount of
ionization they produce in a gas. X-ray quanta can cause ionization just as high-
speed electrons can, namely, by knocking an electron out of a gas molecule and
leaving ...
Ionization devices measure the intensity of x-ray beams by the amount of
ionization they produce in a gas. X-ray quanta can cause ionization just as high-
speed electrons can, namely, by knocking an electron out of a gas molecule and
leaving ...
Page 402
1 that any element, if made the target in an x-ray tube and bombarded with
electrons of high enough energy, would emit a characteristic line spectrum. The
most intense lines of this spectrum are the Ko, and K3 lines. They are always
called ...
1 that any element, if made the target in an x-ray tube and bombarded with
electrons of high enough energy, would emit a characteristic line spectrum. The
most intense lines of this spectrum are the Ko, and K3 lines. They are always
called ...
What people are saying - Write a review
LibraryThing Review
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 | |
23 other sections not shown
Other editions - View all
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 |