## Treatise on materials science and technology, Volume 3 |

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Page 11

In order to make practical calculations it is convenient to work with the

components of the

-(ff21«l + ff22«2 + ff23«3) (53) £3 = -(ff3l«l + ^32«2 + ^33«3)- From Eq. (53) it

follows that ...

In order to make practical calculations it is convenient to work with the

components of the

**energy**-**flux vector**in the form El = -(ffll«l + ffl2«2 + ffl3«3) E2 =-(ff21«l + ff22«2 + ff23«3) (53) £3 = -(ff3l«l + ^32«2 + ^33«3)- From Eq. (53) it

follows that ...

Page 28

Note that the condition for pure mode transverse waves x+f}+y = 0 now becomes /

= 0. (151) Using Eqs. (134), (146), and (150), the components of the

Note that the condition for pure mode transverse waves x+f}+y = 0 now becomes /

= 0. (151) Using Eqs. (134), (146), and (150), the components of the

**energy**-**flux****vector**for transverse waves with respect to the new coordinates are ...Page 34

Deviation of

for aluminum [after Hinton and Green (45)]. normal. It can readily be seen from

Fig. 9 that only at the corners of the standard triangle are the modes of wave ...

Deviation of

**energy**-**flux vectors**from wave normals for quasitransverse waves v3for aluminum [after Hinton and Green (45)]. normal. It can readily be seen from

Fig. 9 that only at the corners of the standard triangle are the modes of wave ...

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