Treatise on Materials Science and Technology, Volume 1 |
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Page 8
81 Å Surface Ergs / ion ( * 1012 ) Kcal / mole NaCl ( smooth cubic face ) 7 . 8 0 .
54 ~ 1 . 0 ~ 15 7 . 15 EC NaCl , cubic face ( H - crystal position ) EA + EA Metal
Surface ( Eb ) . Dielectric Surface EA ( K = 1 . 5 ) ( K = 10 ) ( K = 110 ) 103 29 . 5 2
.
81 Å Surface Ergs / ion ( * 1012 ) Kcal / mole NaCl ( smooth cubic face ) 7 . 8 0 .
54 ~ 1 . 0 ~ 15 7 . 15 EC NaCl , cubic face ( H - crystal position ) EA + EA Metal
Surface ( Eb ) . Dielectric Surface EA ( K = 1 . 5 ) ( K = 10 ) ( K = 110 ) 103 29 . 5 2
.
Page 44
Next , Mullins ( 1959 ) and Mutaftschiev and Kern ( 1964 , 1965 ) made
contributions to the three - level model and , most recently , Temkin ( 1966 )
developed the N - level model for a simple cubic lattice predicting the same
general features as ...
Next , Mullins ( 1959 ) and Mutaftschiev and Kern ( 1964 , 1965 ) made
contributions to the three - level model and , most recently , Temkin ( 1966 )
developed the N - level model for a simple cubic lattice predicting the same
general features as ...
Page 49
We shall initially restrict our attention to a simple cubic solid with a similarly
structured liquid at the equilibrium melting temperature ( T ; = Te ) and will
consider the interface in Fig . 24 as the degree of diffuseness changes . The
interface ...
We shall initially restrict our attention to a simple cubic solid with a similarly
structured liquid at the equilibrium melting temperature ( T ; = Te ) and will
consider the interface in Fig . 24 as the degree of diffuseness changes . The
interface ...
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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