Treatise on Materials Science and Technology, Volume 1 |
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Page 49
THE SURFACE ENERGY - BOND MODEL In this section , we shall first consider
the structure of an infinite surface between a pure solid and its melt for the case
where the interface contains no layer edges . We shall initially restrict our ...
THE SURFACE ENERGY - BOND MODEL In this section , we shall first consider
the structure of an infinite surface between a pure solid and its melt for the case
where the interface contains no layer edges . We shall initially restrict our ...
Page 57
Thus , a proper model of a solid - liquid transitional interface must concern itself
with the existence and development of communal entropy in the interface region
in order to have a basis for being physically and numerically relevant . The major
...
Thus , a proper model of a solid - liquid transitional interface must concern itself
with the existence and development of communal entropy in the interface region
in order to have a basis for being physically and numerically relevant . The major
...
Page 59
A molecule is not incorporated into the solid , and a surface undergoes no
change , except during the passage of a step , i . e . , a molecule can attach itself
to the solid only at the edge of a step . Then , the surface advances normal to
itself by n ...
A molecule is not incorporated into the solid , and a surface undergoes no
change , except during the passage of a step , i . e . , a molecule can attach itself
to the solid only at the edge of a step . Then , the surface advances normal to
itself by n ...
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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