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

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Page 82

It is possible to view this

another way as well. By a linear

that for any level of applied stress a

critical ...

It is possible to view this

**fracture**process in strongly coupled composites inanother way as well. By a linear

**fracture**mechanics approach, it can be expectedthat for any level of applied stress a

**fracture**instability is possible if a certaincritical ...

Page 89

number r of adjacent

of the flaw distribution. Stress enhancement factors Ku K2, and K3 have been

calculated by Scop and Argon (1969) for elastic and plastic matrices for several ...

number r of adjacent

**fractured**elements, but do not depend on the scale factor Cof the flaw distribution. Stress enhancement factors Ku K2, and K3 have been

calculated by Scop and Argon (1969) for elastic and plastic matrices for several ...

Page 110

of the strength maximum, the length of the critical crack for

decreases with increasing exponent m (decreasing element variability). This

increase is partly due to the rise in the composite strength with increasing m. As

the last ...

of the strength maximum, the length of the critical crack for

**fracture**instabilitydecreases with increasing exponent m (decreasing element variability). This

increase is partly due to the rise in the composite strength with increasing m. As

the last ...

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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