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

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Page 42

This produces a nonrandom distribution in the interplanar spacing , which is

related to any texture developed during the plastic deformation process . Marion

and Cohen ( 1974 ) developed a distribution

variation in ...

This produces a nonrandom distribution in the interplanar spacing , which is

related to any texture developed during the plastic deformation process . Marion

and Cohen ( 1974 ) developed a distribution

**function**f ( 4 ) describing thevariation in ...

Page 43

The distribution

obtained by measuring the texture only in the region of the pole figure for which

the residual lattice strain is measured . This is readily accomplished by simply ...

The distribution

**function**describes the variation of d with orientation and isobtained by measuring the texture only in the region of the pole figure for which

the residual lattice strain is measured . This is readily accomplished by simply ...

Page 121

Finally for a disordered magnetic alloy where there may exist a continuous

distribution of hyperfine fields represented by a probability

coefficients of ...

Finally for a disordered magnetic alloy where there may exist a continuous

distribution of hyperfine fields represented by a probability

**function**P ( H ) , this**function**may be approximated by a set of trigonometrical**functions**thecoefficients of ...

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### Contents

The Investigation of Composition | 63 |

Penetration Distance | 75 |

Choice of Binary System for Composition | 86 |

Copyright | |

11 other sections not shown

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absorption addition allow alloy angle Appl applications atoms band bandgap beam broadening coefficients components composition concentration containing cooling copper cross section curve deep defects dependent deposits depth determined developed diffraction diffusion direction discussed dislocation distribution donor effect electron elements emission energy et al example excitation experimental factor field function give given heat hyperfine important impurities increasing intensity interaction iron laser lattice layer less magnetic material measurements Metals method Monemar Mössbauer neighbor observed obtained occur optical parameter peak phase Phys position possible powders problem produce properties range rays recently recombination region relative ribbon sample semiconductors shift shown solid spacing specimen spectra spectrum sputtering steel stress structure studies substrate surface target techniques temperature term thickness values variation volume X-ray