Treatise on Materials Science and Technology, Volume 1 |
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Page 2
In order to progress further in this area , it is necessary to follow a path of study
aimed at revealing the individual factors which determine the interfacial energy
and the interface configuration between any two materials . To illustrate the
various ...
In order to progress further in this area , it is necessary to follow a path of study
aimed at revealing the individual factors which determine the interfacial energy
and the interface configuration between any two materials . To illustrate the
various ...
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 260
This assumption is necessary so that each element of surface on the original
interface can be unambiguously associated with an element on the displaced
surface . This one - to - one association is accomplished by constructing normals
to the ...
This assumption is necessary so that each element of surface on the original
interface can be unambiguously associated with an element on the displaced
surface . This one - to - one association is accomplished by constructing normals
to 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