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

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Page 52

25

05 and 0 . 02 for Sn and Ge , respectively . This procedure illustrates the method

of evaluating & z / kTe and X * for a particular system ; however , the magnitudes

...

25

**gives**€1 / kTe ~ 0 . 8 and 1 for Sn and Ge , respectively . It also**gives**X * ~ 0 .05 and 0 . 02 for Sn and Ge , respectively . This procedure illustrates the method

of evaluating & z / kTe and X * for a particular system ; however , the magnitudes

...

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

values of 0 , otherwise this approach can

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 338

010 inches of the substrate . This has only just recently been proved by X - ray

textural studies as a function of distance from the substrate for different deposition

temperatures ( Shim , 1971 ) . At 500° C the randomness

010 inches of the substrate . This has only just recently been proved by X - ray

textural studies as a function of distance from the substrate for different deposition

temperatures ( Shim , 1971 ) . At 500° C the randomness

**gives**way within 0 .### What people are saying - Write a review

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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