Treatise on Materials Science and Technology, Volume 1 |
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Page 8
The interaction energy of the ion and the atom due to this electrostatic
polarization is Ea = - ( az ? r - 4 / 2 ) ( 5b ) Equation ( 5b ) gives the contribution
toward the adsorption energy of an ion , on a condensed phase , by the
polarization of only ...
The interaction energy of the ion and the atom due to this electrostatic
polarization is Ea = - ( az ? r - 4 / 2 ) ( 5b ) Equation ( 5b ) gives the contribution
toward the adsorption energy of an ion , on a condensed phase , by the
polarization of only ...
Page 11
FREE ELECTRON ENERGY STATES A contribution to yc is expected to arise
from the change in the kinetic energy of the electrons due to the different volume
available for them at the surface and due to the penetration of the surface by the ...
FREE ELECTRON ENERGY STATES A contribution to yc is expected to arise
from the change in the kinetic energy of the electrons due to the different volume
available for them at the surface and due to the penetration of the surface by the ...
Page 171
This occurs because C33 is very much larger than cu or C44 . For most values of
0k , the wave propagation is determined by C33 which has a nondispersive
contribution . For Ox = 90° , the contribution of cu or C44 becomes comparable to
that ...
This occurs because C33 is very much larger than cu or C44 . For most values of
0k , the wave propagation is determined by C33 which has a nondispersive
contribution . For Ox = 90° , the contribution of cu or C44 becomes comparable to
that ...
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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