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

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Page 122

Thus , we can restrict the force

may have to include the effect of several neighbors because the elastic

disturbances in the matrix may extend quite far . However , the number of

neighbors to be ...

Thus , we can restrict the force

**constants**to few near neighbors . In practice , onemay have to include the effect of several neighbors because the elastic

disturbances in the matrix may extend quite far . However , the number of

neighbors to be ...

Page 132

Equating the coefficients of k ; ? in the corresponding elements of the matrices D (

k ) and A ( k ) , we get the following relations between the force

elastic

Equating the coefficients of k ; ? in the corresponding elements of the matrices D (

k ) and A ( k ) , we get the following relations between the force

**constants**and theelastic

**constants**A + 2D = ( 11 B + 2D = 266 E = C44 F + 2G = C44 ( 50 ) H ...Page 169

Herbert Herman. Let us consider a wave traveling in the yz plane . For this plane

the form of the dispersion relations will be the same for tetragonal and hexagonal

symmetries . Using the Set 1 for the elastic

Herbert Herman. Let us consider a wave traveling in the yz plane . For this plane

the form of the dispersion relations will be the same for tetragonal and hexagonal

symmetries . Using the Set 1 for the elastic

**constants**( Section X ) , and p = 2 , E ...### 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