Treatise on Materials Science and Technology, Volume 1 |
From inside the book
Results 1-3 of 28
Page 133
The three eigenvalues of the dynamical matrix for a value of k give the
frequencies of the three types of waves , and the corresponding eigenvectors
describe the polarization of those three waves . If li denote the three Cartesian
components ( i ...
The three eigenvalues of the dynamical matrix for a value of k give the
frequencies of the three types of waves , and the corresponding eigenvectors
describe the polarization of those three waves . If li denote the three Cartesian
components ( i ...
Page 135
... ( k ) = 4K sin kį sin k2 ( 59 ) D22 ( k ) = 2A ( 1 – coska ) + 2B ( 1 - coski ) + 4D ( 1
- cosk , coska ) and D ' ( k ) = 2F ( 2 - cosk , - coską ) + 4G ( 1 – cosk , cosk2 ) ( 60
) The eigenvalue corresponding to the element DTM ( k ) is immediately known ...
... ( k ) = 4K sin kį sin k2 ( 59 ) D22 ( k ) = 2A ( 1 – coska ) + 2B ( 1 - coski ) + 4D ( 1
- cosk , coska ) and D ' ( k ) = 2F ( 2 - cosk , - coską ) + 4G ( 1 – cosk , cosk2 ) ( 60
) The eigenvalue corresponding to the element DTM ( k ) is immediately known ...
Page 145
... one of the eigenvalues , the one corresponding to D * is immediately known . It
is given by x2 = 2066 ( 1 - сos k2 ) + C44 k 32 ( 82 ) The eigenvector
corresponding to this eigenvalue is [ 1 , 0 , 0 ] . This wave is always polarized
perpendicular ...
... one of the eigenvalues , the one corresponding to D * is immediately known . It
is given by x2 = 2066 ( 1 - сos k2 ) + C44 k 32 ( 82 ) The eigenvector
corresponding to this eigenvalue is [ 1 , 0 , 0 ] . This wave is always polarized
perpendicular ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Other editions - View all
Common terms and phrases
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