Treatise on Materials Science and Technology, Volume 1 |
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Page 84
... + V , E , VEL 400 = " < m a cam where V , is the volume fraction of the
reinforcing material , Gm the shear modulus of the matrix material , E , the Young '
s modulus of the reinforcing material , and k , = o vc is the Mode I stress intensity
factor .
... + V , E , VEL 400 = " < m a cam where V , is the volume fraction of the
reinforcing material , Gm the shear modulus of the matrix material , E , the Young '
s modulus of the reinforcing material , and k , = o vc is the Mode I stress intensity
factor .
Page 333
Microhardness traverses have been run radially , through the tube thickness , on
surfaces cut normal to the tube axis for each substrate temperature . It is found
that the material produced at the 500° C substrate temperature is the harder of
the ...
Microhardness traverses have been run radially , through the tube thickness , on
surfaces cut normal to the tube axis for each substrate temperature . It is found
that the material produced at the 500° C substrate temperature is the harder of
the ...
Page 338
Grain growth in CVD materials is intimately connected with the development of
bubbles and their subsequent interaction with migrating grain boundaries . We
have only noticed that for higher temperature anneals , plots of D2 – D . 2 versus
...
Grain growth in CVD materials is intimately connected with the development of
bubbles and their subsequent interaction with migrating grain boundaries . We
have only noticed that for higher temperature anneals , plots of D2 – D . 2 versus
...
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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