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

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Page 137

Figure 13 defines the magnitude of t* at temperature Tl as T*r t* becomes zero at

a critical temperature, Tc, where the magnitude of

enough to provide sufficient

obstacles ...

Figure 13 defines the magnitude of t* at temperature Tl as T*r t* becomes zero at

a critical temperature, Tc, where the magnitude of

**thermal**fluctuations is largeenough to provide sufficient

**thermal**energy to overcome the short-rangeobstacles ...

Page 146

As the distance from the core, R, becomes large, HelastU and He1cctric become

very small. Because of this (l/R) dependence,

lattice strongly influence the magnitude of Helastic and //electric sucn tnat they

have ...

As the distance from the core, R, becomes large, HelastU and He1cctric become

very small. Because of this (l/R) dependence,

**thermal**fluctuations in the alloylattice strongly influence the magnitude of Helastic and //electric sucn tnat they

have ...

Page 322

... 116-120, 131, 135, 150 Strain aging, 132-133 Strain broadening, 51

Substrates, thin films, 1 1 Suzuki interaction, 150 Textured polycrystalline films,

35

Thermodynamics, ...

... 116-120, 131, 135, 150 Strain aging, 132-133 Strain broadening, 51

Substrates, thin films, 1 1 Suzuki interaction, 150 Textured polycrystalline films,

35

**Thermal**diffusion, 110**Thermal**fluctuation, 147**Thermal**strains, 115Thermodynamics, ...

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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