## Treatise on materials science and technology, Volume 1 |

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Page 276

In a nucleation and growth process, this occurs after roughly 0.1 of the volume

has transformed to the new phase. At this stage a significant number of growing

grains will have encountered each other. This

...

In a nucleation and growth process, this occurs after roughly 0.1 of the volume

has transformed to the new phase. At this stage a significant number of growing

grains will have encountered each other. This

**impingement**process produces PP...

Page 278

This is the basic equation governing uniform

equation yields Vy = 1 -exp(-Fvex) (42) It is clear that this result has the proper

general form required, since as t -» oo and Vyex-* oo,Fv-> 1. The value of Fvex

may be ...

This is the basic equation governing uniform

**impingement**. Integration of thisequation yields Vy = 1 -exp(-Fvex) (42) It is clear that this result has the proper

general form required, since as t -» oo and Vyex-* oo,Fv-> 1. The value of Fvex

may be ...

Page 280

B. The General

behavior in complex systems to physical models probably arises from an

inadequate description of the effects of

upon the ...

B. The General

**Impingement**Problem Much of the difficulty of fitting observedbehavior in complex systems to physical models probably arises from an

inadequate description of the effects of

**impingement**of the growing particlesupon the ...

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activation energy alloys angle annealing Argon Arsenault axis binding energy bond calculated carbon chemical vapor deposition crystal curvature curve CVD tungsten Debye decrease deposition determined dipole displacement distribution effect elastic constants elastic waves electron equation equilibrium experimental Fe-Mn-N Fe-N fibers force constants fracture free energy function geometric given grain boundaries group velocities growth path envelope Hasson hoop stress impingement increase interface internal friction interstitial ions kcal/mole kinetics laminate lattice layer manganese measured mechanism metal microstructural change molecules neighbors niobium nitrogen nitrogen atoms nucleation obtained oxygen parameters particles peak broadening peak height phase potential propagation reinforcing elements relaxation processes rhenium s-i interaction s-i pair scavenging Section shear shown in Fig Snoek peak solid specimen structure substitutional addition substitutional solute substrate surface tensile ternary alloys tetragonal titanium transverse wave triple line tungsten values vanadium volume fraction xy plane yield stress zirconium