Treatise on Materials Science and Technology, Volume 1 |
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Page 117
characteristic feature of the composite . 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 ...
characteristic feature of the composite . 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 ...
Page 121
For the theoretical treatment given in this paper we shall first assume a perfect
composite . A perfect composite is defined to be one in which all the fibers are of
equal mass and length , extend throughout the length of the composite , have ...
For the theoretical treatment given in this paper we shall first assume a perfect
composite . A perfect composite is defined to be one in which all the fibers are of
equal mass and length , extend throughout the length of the composite , have ...
Page 173
This conclusion has been derived for dispersion curves obtained by neutron
scattering from a crystal lattice and will also apply to some extent to the present
case of the scattering of elastic waves from composites . However , it may be that
the ...
This conclusion has been derived for dispersion curves obtained by neutron
scattering from a crystal lattice and will also apply to some extent to the present
case of the scattering of elastic waves from composites . However , it may be that
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