Treatise on Materials Science and Technology, Volume 1 |
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Page 76
However , if we follow Landau ( 1967 ) and restrict our attention to the interaction
between two electrically neutral groups of atoms at a distance d via van der
Waals attractive forces , then the layers repel each other . To see this , consider
the ...
However , if we follow Landau ( 1967 ) and restrict our attention to the interaction
between two electrically neutral groups of atoms at a distance d via van der
Waals attractive forces , then the layers repel each other . To see this , consider
the ...
Page 191
similar to the aforementioned Fe - V - N type s - i interactions . The variation with
interstitial ... The model for the Fe - V - N interaction presently involves an attempt
to explain the high temperature peak . The applicability and exactness of this ...
similar to the aforementioned Fe - V - N type s - i interactions . The variation with
interstitial ... The model for the Fe - V - N interaction presently involves an attempt
to explain the high temperature peak . The applicability and exactness of this ...
Page 225
28 where lines from the solvent indicate whether scavenging occurs , an săi
interaction is present and responsible for peak broadening ( for Group V alloys
the definition of s - i interactions assumes a broader definition , which includes
the ...
28 where lines from the solvent indicate whether scavenging occurs , an săi
interaction is present and responsible for peak broadening ( for Group V alloys
the definition of s - i interactions assumes a broader definition , which includes
the ...
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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