Treatise on Materials Science and Technology, Volume 1 |
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Page 26
The Galvani potential of a phase cannot be measured and even the Galvani
potential difference between two phases is not ... For such a measurement , it
would be necessary to determine the electrostatic work required to bring a small
charge ...
The Galvani potential of a phase cannot be measured and even the Galvani
potential difference between two phases is not ... For such a measurement , it
would be necessary to determine the electrostatic work required to bring a small
charge ...
Page 169
We can of course determine the experimental values of the elastic constants from
the measured values of the phase velocities . The elastic constants , thus
determined , are given as Set 2 in Section X . The elastic constants C11 , 066 ,
044 ...
We can of course determine the experimental values of the elastic constants from
the measured values of the phase velocities . The elastic constants , thus
determined , are given as Set 2 in Section X . The elastic constants C11 , 066 ,
044 ...
Page 173
Some estimate of the force constants can also be obtained by a measurement of
the thermodynamic quantities . The calculation of ... ( 1 ) The bonding strength of
the fibers in a composite can be measured by using short elastic waves .
Some estimate of the force constants can also be obtained by a measurement of
the thermodynamic quantities . The calculation of ... ( 1 ) The bonding strength of
the fibers in a composite can be measured by using short elastic waves .
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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