## Treatise on materials science and technology, Volume 4 |

### From inside the book

Results 1-3 of 27

Page 89

Now the yth

also has a nonzero x projection, may be of type a, or any other jump type for that

matter. Furthermore, this jump could have either the same or the opposite x ...

Now the yth

**tracer jump**with nonzero x projection following one of type a, whichalso has a nonzero x projection, may be of type a, or any other jump type for that

matter. Furthermore, this jump could have either the same or the opposite x ...

Page 92

Namely, if the solvent

specifies the position of the

position of the solute determines the

...

Namely, if the solvent

**tracer**position is fixed and the vacancy**jump**into the**tracer**specifies the position of the

**tracer**and vacancy following the**jump**, the relativeposition of the solute determines the

**jump**type. For diffusion in the fcc lattice with...

Page 105

That is, when a new vacancy (one which has not exchanged with the tracer)

becomes a neighbor with the tracer and makes a diffusive jump, P is the net

effective probability that the next

plane.

That is, when a new vacancy (one which has not exchanged with the tracer)

becomes a neighbor with the tracer and makes a diffusive jump, P is the net

effective probability that the next

**tracer jump**will return the tracer to the original xplane.

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### Contents

Microstructural Characterization of Thin Films | 2 |

Fundamental Concepts of Diffraction | 4 |

Epitaxial Monocrystalline Films | 10 |

Copyright | |

26 other sections not shown

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### Common terms and phrases

a-sublattice Acta alloys aluminum average beam calculated compaction component compositional dependences compression concentration configurational entropy copper correlation factor crystallites CsCl phases decreases deformation diffraction pattern diffusion coefficient dislocation density disorder parameter effect electron diffraction equations Evans and Flanagan f.c. tetragonal face-centered cubic fiber axis flux forged free energy function Gibbs free energy given increases intermetallic iron powder isostatic jump rate lattice disorder material matrix mechanism nearest neighbor observed obtained occurs oriented partial enthalpy partial entropy Phys plane Poisson ratio polycrystalline probability pure metals random reciprocal lattice relps RHEED shear stress shown in Fig single crystals sintered sintered powder solid solution strengthening solute atoms solute content specimen stacking fault energy stoichiometry stress-strain curve structure sublattice Substituting surface Suzuki TED pattern temperature dependence tetragonal theoretical thermal thermodynamic thermodynamic activities thermodynamic properties thin films tracer jump twin vacancy jumps values variations Vook X-ray yield stress