## Treatise on Materials Science and Technology, Volume 1 |

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Page 33

In Table V

given for a number of metals . These

reasons : our choice of £ * , our use of the condenser approximation , the Eq ...

In Table V

**values**of Adsl and lyel , as well as the experimental**values**of YsL , aregiven for a number of metals . These

**values**may be somewhat in error for severalreasons : our choice of £ * , our use of the condenser approximation , the Eq ...

Page 153

As the Fourier coefficients are very sensitive to the details of the function , it is

very important for this technique that E ( 0 ) is accurately measured for many

As the Fourier coefficients are very sensitive to the details of the function , it is

very important for this technique that E ( 0 ) is accurately measured for many

**values**of 0 , otherwise this approach can give results which are wildly in error .Page 169

One possible explanation could be that the calculated

constants do not agree with the actual elastic constants of the sample used for

the experiments . We can of course determine the experimental

elastic ...

One possible explanation could be that the calculated

**values**of the elasticconstants do not agree with the actual elastic constants of the sample used for

the experiments . We can of course determine the experimental

**values**of theelastic ...

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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