Treatise on Materials Science and Technology, Volume 1 |
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Page 43
Representation of the different , energetically unique , surface sites for molecules
. of new , unique energy states that ... To better appreciate the different states of
molecular attachment between one condensed phase and another , let us first ...
Representation of the different , energetically unique , surface sites for molecules
. of new , unique energy states that ... To better appreciate the different states of
molecular attachment between one condensed phase and another , let us first ...
Page 46
two , three , or more molecules and vacancies appear on the surface . At still
higher temperatures , if the crystal has not melted , more than three levels are
involved . This progressive roughening can be viewed as a cooperative
disordering of ...
two , three , or more molecules and vacancies appear on the surface . At still
higher temperatures , if the crystal has not melted , more than three levels are
involved . This progressive roughening can be viewed as a cooperative
disordering of ...
Page 49
24a exhibits zero diffuseness and consists of “ solid ” molecules in state 0 ( Fig .
22 ) , whereas in Fig . 24b and 24c , the “ solid ” molecules are in + 1 states and +
1 , + 2 states , respectively . We shall first deduce the excess free energy per site
...
24a exhibits zero diffuseness and consists of “ solid ” molecules in state 0 ( Fig .
22 ) , whereas in Fig . 24b and 24c , the “ solid ” molecules are in + 1 states and +
1 , + 2 states , respectively . We shall first deduce the excess free energy per site
...
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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