Treatise on Materials Science and Technology, Volume 1 |
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Page 117
On a plane perpendicular to the fibers the present model behaves like a discrete
crystal lattice , whereas it behaves like a Debye elastic continuum in a direction
parallel to the fibers . This is physically reasonable for a composite because the ...
On a plane perpendicular to the fibers the present model behaves like a discrete
crystal lattice , whereas it behaves like a Debye elastic continuum in a direction
parallel to the fibers . This is physically reasonable for a composite because the ...
Page 121
A perfect composite is defined to be one in which all the fibers are of equal mass
and length , extend throughout the ... Note , that for the treatment given here it is
not essential to assume that the bonding between the fibers and the matrix is ...
A perfect composite is defined to be one in which all the fibers are of equal mass
and length , extend throughout the ... Note , that for the treatment given here it is
not essential to assume that the bonding between the fibers and the matrix is ...
Page 173
This is because the elastic displacements of fibers can be determined from the
theory of elasticity unlike the atomic displacements in a crystal lattice . Finally ,
the main results of the present paper are as follows . ( 1 ) The bonding strength of
the ...
This is because the elastic displacements of fibers can be determined from the
theory of elasticity unlike the atomic displacements in a crystal lattice . Finally ,
the main results of the present paper are as follows . ( 1 ) The bonding strength of
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