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

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Page 122

The intensity of each subspectrum is a function of

for a random alloy is given by 12 ! P ( n ) = ( 7 ) ( 12 - ni ni c ( 1 - c ) 12 - n where n

is the number of nearest neighbor B atoms . Although the crystal symmetry ...

The intensity of each subspectrum is a function of

**concentration**c of B atoms andfor a random alloy is given by 12 ! P ( n ) = ( 7 ) ( 12 - ni ni c ( 1 - c ) 12 - n where n

is the number of nearest neighbor B atoms . Although the crystal symmetry ...

Page 130

The use of a consistent model to fit spectra over a range of carbon

adds weight to the component ... fields at 269 and 348 k0e , whose relative

intensities were proportional to 2c and 4c , where c is the carbon

The use of a consistent model to fit spectra over a range of carbon

**concentrations**adds weight to the component ... fields at 269 and 348 k0e , whose relative

intensities were proportional to 2c and 4c , where c is the carbon

**concentration**.Page 143

Hence , in order to determine the phase

know the composition and recoiless fraction ... It is due probably to the filling of

the d states with increasing europium

the ...

Hence , in order to determine the phase

**concentrations**in a mixture , we need toknow the composition and recoiless fraction ... It is due probably to the filling of

the d states with increasing europium

**concentration**leading to an expansion inthe ...

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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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### Common terms and phrases

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