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

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Page 93

The only difference here is that these " particles " must be followed by

walk. These are the vacancy, the solute atom, and the tracer jumps with zero x

projection. As before configurations of the particles can be reduced by symmetry.

The only difference here is that these " particles " must be followed by

**random**walk. These are the vacancy, the solute atom, and the tracer jumps with zero x

projection. As before configurations of the particles can be reduced by symmetry.

Page 103

Other Forces To this point, the description has attempted to show the influences

that the

approach, the development of Eq. (24) using the jump rate between two adjacent

...

Other Forces To this point, the description has attempted to show the influences

that the

**random**walk of vacancies can have on the diffusion coefficient. In thisapproach, the development of Eq. (24) using the jump rate between two adjacent

...

Page 126

Order Average Number of Unlike Neighbors =4 Clustering Average Number of

Unlike Neighbors =2 Fig. 5. Two-dimensional illustration of (a)

**Random**Solution Average Number of Unlike Neighbors =3 a = 0 Short RangeOrder Average Number of Unlike Neighbors =4 Clustering Average Number of

Unlike Neighbors =2 Fig. 5. Two-dimensional illustration of (a)

**random**solution, ...### What people are saying - Write a review

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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