Treatise on Materials Science and Technology, Volume 1 |
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Page 36
In general , one would expect atoms with many electrons to have a larger
polarizability a than those with few electrons ... This is because of the screening
charge surrounding the solute atom which exhibits charge oscillations out to radii
of ...
In general , one would expect atoms with many electrons to have a larger
polarizability a than those with few electrons ... This is because of the screening
charge surrounding the solute atom which exhibits charge oscillations out to radii
of ...
Page 184
They may be thought to comprise three equivalent sets , coordinated by atoms in
the X , Y , and Z directions , respectively . Ordinarily , interstitial solute atoms
occupy all sets with equal probability ; however , this random distribution can be ...
They may be thought to comprise three equivalent sets , coordinated by atoms in
the X , Y , and Z directions , respectively . Ordinarily , interstitial solute atoms
occupy all sets with equal probability ; however , this random distribution can be ...
Page 231
32 ) for a nitrogen atom leaving the Mn couple , is due to the prohibitively high
activation energy and may also be due to the ... Model for the interaction between
nitrogen and manganese solute atoms in iron ( Gladman and Pickering , 1965 ) .
32 ) for a nitrogen atom leaving the Mn couple , is due to the prohibitively high
activation energy and may also be due to the ... Model for the interaction between
nitrogen and manganese solute atoms in iron ( Gladman and Pickering , 1965 ) .
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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