Treatise on Materials Science and Technology, Volume 1 |
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Page 2
We make imaginary cuts through the cross section of each crystal and separate
the halves of each crystal without allowing either atomic or electronic ... We next
bring the a and ß half - crystals together along the cut surfaces gaining work Web
.
We make imaginary cuts through the cross section of each crystal and separate
the halves of each crystal without allowing either atomic or electronic ... We next
bring the a and ß half - crystals together along the cut surfaces gaining work Web
.
Page 7
DIRECT COULOMB FORCES If we idealize the surface of an ionic compound ( e
. g . , alkali halide crystal ) as a two - dimensional network of ions and we assume
a negative ion adsorbed just on top of one of the positive ions of the surface ...
DIRECT COULOMB FORCES If we idealize the surface of an ionic compound ( e
. g . , alkali halide crystal ) as a two - dimensional network of ions and we assume
a negative ion adsorbed just on top of one of the positive ions of the surface ...
Page 43
We shall regard the crystal as a simple cubic lattice for the sake of illustration , the
sites of which are occupied by molecules . Depicting the molecules as cubes ,
typical situations for surface molecules will be as illustrated in Fig . 22 . Molecules
...
We shall regard the crystal as a simple cubic lattice for the sake of illustration , the
sites of which are occupied by molecules . Depicting the molecules as cubes ,
typical situations for surface molecules will be as illustrated in Fig . 22 . Molecules
...
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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