Treatise on Materials Science and Technology, Volume 1 |
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Page 113
The energy due to the double bending of the lamellae can be calculated readily
by the well - known formula for bending slender beams and is AEZ = cE , 1 ( 40 ) /
bt , ( 1 – 12 ) ( A - 5 ) where E , is the Young ' s modulus of the reinforcement ...
The energy due to the double bending of the lamellae can be calculated readily
by the well - known formula for bending slender beams and is AEZ = cE , 1 ( 40 ) /
bt , ( 1 – 12 ) ( A - 5 ) where E , is the Young ' s modulus of the reinforcement ...
Page 117
The present model for a composite is “ dispersive " for short waves in the same
sense as the Born - von Karman model is for the electromagnetic waves ( neutron
beams , X rays ) . The limiting case of long waves is obtained by using Born ' s ...
The present model for a composite is “ dispersive " for short waves in the same
sense as the Born - von Karman model is for the electromagnetic waves ( neutron
beams , X rays ) . The limiting case of long waves is obtained by using Born ' s ...
Page 172
For most angles of incidence the p , wave is polarized in a direction close to the
fiber axis ( Figs . 13 and 23 ) , and thus on traveling through a composite , the
original set of elastic waves will emerge as a highly collimated beam of more or
less ...
For most angles of incidence the p , wave is polarized in a direction close to the
fiber axis ( Figs . 13 and 23 ) , and thus on traveling through a composite , the
original set of elastic waves will emerge as a highly collimated beam of more or
less ...
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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