## Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |

### From inside the book

Results 1-3 of 48

Page 8

Herbert Herman. then m ' ( 5b ) dy , v = o [ ( 1 + v ) / E ] Because several

d pob are determined , errors resulting from random fluctuations are minimized .

Four to six y tilts , taken in equal increments of sina y , are normally employed .

Herbert Herman. then m ' ( 5b ) dy , v = o [ ( 1 + v ) / E ] Because several

**values**ofd pob are determined , errors resulting from random fluctuations are minimized .

Four to six y tilts , taken in equal increments of sina y , are normally employed .

Page 13

The analysis is based on strains ( eu ) and primes imply

coordinates , whereas unprimed quantities refer to the specimen axes . For

example , €33 is the strain normal to the diffracting planes €33 ( 4 , 4 ) = devo - do

= €33 ...

The analysis is based on strains ( eu ) and primes imply

**values**in laboratorycoordinates , whereas unprimed quantities refer to the specimen axes . For

example , €33 is the strain normal to the diffracting planes €33 ( 4 , 4 ) = devo - do

= €33 ...

Page 85

The endpoints are 8 functions with appropriate integral

neglects sample absorption ... A single g

of the original specimen interface . If g were to take on different

The endpoints are 8 functions with appropriate integral

**values**. The solid curveneglects sample absorption ... A single g

**value**has been assumed for both sidesof the original specimen interface . If g were to take on different

**values**on each ...### What people are saying - Write a review

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### Contents

R JAMES | 2 |

Principles of XRay Stress Measurement | 4 |

Control of Accuracy and Precision | 25 |

Copyright | |

15 other sections not shown

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absorption additional allows alloy angle Appl applications atoms bandgap beam broadening cause coefficients components composition composition profile concentration constant containing cooling crystal curve defects dependent deposits depth determined developed diffraction diffusion direction discussed dislocation distance distribution effect electron elements employed energy error et al example excitation experimental factor field function give given grain heat important included increasing intensity intensity bands iron laser lattice layer less magnetic material measurements Metals method Mössbauer observed obtained occur optical parameter peak phase Phys plane position possible powder problem produce range rays recent region relative residual stress sample semiconductors shift shown single Society solid spacing specimen spectra spectrum sputtering steel structure studies substrate surface target technique temperature term thickness values variation volume x-ray