Treatise on Materials Science and Technology, Volume 1 |
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Page 34
... both the charge density o and excess energy ve become more characteristic of
phase II as a homogeneous capacitor . ... be excellent when the film is very thin
and that it may strongly decrease as the film thickness becomes larger than 2d , .
... both the charge density o and excess energy ve become more characteristic of
phase II as a homogeneous capacitor . ... be excellent when the film is very thin
and that it may strongly decrease as the film thickness becomes larger than 2d , .
Page 69
In the time At , this becomes segment cd . Thus AA = cd - ab and AV = abcd . The
segment ef is what ab would have become if the surface grew as a cylinder
instead of translating in the Z direction at constant velocity V . It is apparent that
cd ...
In the time At , this becomes segment cd . Thus AA = cd - ab and AV = abcd . The
segment ef is what ab would have become if the surface grew as a cylinder
instead of translating in the Z direction at constant velocity V . It is apparent that
cd ...
Page 71
Of course , it can be properly argued that 8 = 0 at the instability limit ; however , to
observe any physical manifestations of instability Š > 0 and the second term in Eq
. ( 77 ) becomes significant . Perhaps the most important consequence of this ...
Of course , it can be properly argued that 8 = 0 at the instability limit ; however , to
observe any physical manifestations of instability Š > 0 and the second term in Eq
. ( 77 ) becomes significant . Perhaps the most important consequence of this ...
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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