Treatise on Materials Science and Technology, Volume 1 |
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Page 183
Interstitial sites and diffusion paths in a bcc alloy for ( a ) no applied stress and ( b
) with an applied stress . the problem ( e . g . , the mode can be different for an
interstitial in the neighborhood of a solvent atom than for a substitutional solute ...
Interstitial sites and diffusion paths in a bcc alloy for ( a ) no applied stress and ( b
) with an applied stress . the problem ( e . g . , the mode can be different for an
interstitial in the neighborhood of a solvent atom than for a substitutional solute ...
Page 185
Here the applied stress cycle is short enough for the anelastic ( i . e . ,
timedependent ) strain to have a finite value , while the stress variation is not
short enough for equilibrium to be reached . Under this condition , the anelastic
strain does not ...
Here the applied stress cycle is short enough for the anelastic ( i . e . ,
timedependent ) strain to have a finite value , while the stress variation is not
short enough for equilibrium to be reached . Under this condition , the anelastic
strain does not ...
Page 336
We then would have a true representation of oa = KA20 a and the slope K may
be directly applied to subsequently measured values of A20 from other CVD
tungsten tubes . The only distinction then will be that we will be measuring a
Oresidual ...
We then would have a true representation of oa = KA20 a and the slope K may
be directly applied to subsequently measured values of A20 from other CVD
tungsten tubes . The only distinction then will be that we will be measuring a
Oresidual ...
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addition alloys analysis angle applied approach associated assumed atoms average becomes bond boundary calculated complex composite concentration consider constants contribution crystal curvature curve decrease defined dependence deposition determined developed direction discussed displacement distance distribution dynamical effect elastic electron elements energy equal equation exist experimental fibers force fracture function given gives grain grain boundaries Group growth growth path illustrated increase indicate interaction interface internal friction interstitial iron laminate lattice layer length material matrix measured mechanism metal microstructural molecules nitrogen normal nucleation observed obtained occur oxygen particles peak phase plane position possible potential present produce properties region reinforcing relaxation respectively shown in Fig shows single Snoek peak solid solution strain strength stress structure substitutional surface Table temperature tungsten unit values volume waves