Treatise on Materials Science and Technology, Volume 1 |
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Page 34
However , as the slab decreases in thickness below twice the Debye length 2dı ,
the space charge distribution must ... may be excellent when the film is very thin
and that it may strongly decrease as the film thickness becomes larger than 2d , .
However , as the slab decreases in thickness below twice the Debye length 2dı ,
the space charge distribution must ... may be excellent when the film is very thin
and that it may strongly decrease as the film thickness becomes larger than 2d , .
Page 61
Since Ye ' will decrease for re < W / 2 , we should expect re to decrease with
increase of ATX in a classical fashion until it reaches the value of W , 2 and then
to decrease more rapidly with further increase of ATKl . This transition point
occurs at ...
Since Ye ' will decrease for re < W / 2 , we should expect re to decrease with
increase of ATX in a classical fashion until it reaches the value of W , 2 and then
to decrease more rapidly with further increase of ATKl . This transition point
occurs at ...
Page 97
We show first that when the number of elements is very large the laminate
strength decreases monotonically with ... monotonic decrease in the laminate
strength given by Eq . ( 21 ) is primarily a result of the increasingly many sites
from which ...
We show first that when the number of elements is very large the laminate
strength decreases monotonically with ... monotonic decrease in the laminate
strength given by Eq . ( 21 ) is primarily a result of the increasingly many sites
from which ...
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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