## 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 109

The

phase on a

in the figure, however, have a path difference equal to (CB – AD) and are thus.

The

**waves**scattered in the forward direction by electrons A and B are exactly inphase on a

**wave**front such as XX', because ... The other scattered**waves**shownin the figure, however, have a path difference equal to (CB – AD) and are thus.

Page 115

The two

field intensity E with time t of two rays on any given

beam. Their equations may be written E1 = A1 sin (2xvt – £1), (4–5) E2 = A2 ...

The two

**waves**shown as full lines in Fig. 4–10 represent the variations in electricfield intensity E with time t of two rays on any given

**wave**front in a diffracted x-raybeam. Their equations may be written E1 = A1 sin (2xvt – £1), (4–5) E2 = A2 ...

Page 116

2^ (4–8) Thus the

(4–8). The expression on the left is called a complex exponential function. Since

the intensity of a

2^ (4–8) Thus the

**wave**vector may be expressed analytically by either side of Eq.(4–8). The expression on the left is called a complex exponential function. Since

the intensity of a

**wave**is proportional to the square of its amplitude, we now ...### 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

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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 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 slit solid solution spacing specimen stress structure substance surface temperature thickness tion tube twin unit cell usually vector voltage wave wavelength x-ray