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

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Page 8

(33) For a wave to have particle displacements parallel to the surface of the solid

(

= 0. (34) B. Energy Flux Also of great importance to elastic wave propagation in ...

(33) For a wave to have particle displacements parallel to the surface of the solid

(

**pure mode transverse**or shear wave) the condition to be satisfied is al + Pm + yn= 0. (34) B. Energy Flux Also of great importance to elastic wave propagation in ...

Page 34

Deviation of energy-flux vectors from wave normals for quasitransverse waves v3

for aluminum [after Hinton and Green ... At the [100] and [1 10] corners

Deviation of energy-flux vectors from wave normals for quasitransverse waves v3

for aluminum [after Hinton and Green ... At the [100] and [1 10] corners

**pure**-**mode transverse**waves are propagated and there are no energy- flux deviations.Page 51

... pv22, (159) where p is the density and, as was shown in Chapter II, Section III,

vl and v2 are the wave speeds associated with pure mode longitudinal and

... pv22, (159) where p is the density and, as was shown in Chapter II, Section III,

vl and v2 are the wave speeds associated with pure mode longitudinal and

**pure****mode transverse**wave propagation along any direction in an isotropic material.### What people are saying - Write a review

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Alers aluminum Andreatch anisotropic Appl axis calculated compressive stress copper crystallographic orientation cubic crystals determine direction cosines displacement gradients displacements along 001 elastic moduli elastic wave propagation energy-flux vector equation of motion experimental germanium given by Eq hydrostatic pressure hydrostatic pressure longitudinal hydrostatic pressure transverse ideal orientation interaction isotropic solid linear elastic wave longitudinal wave longitudinal wave propagating materials mode transverse wave nonlinear elastic wave obtain Papadakis particle displacements phonons Phys plane wave pressure longitudinal wave pressure transverse wave pure mode longitudinal pure mode transverse quasitransverse waves rolling direction rolling plane second harmonic second-order elastic constants shear wave single crystals six third-order elastic stress along 001 stress along 110 Substituting Eqs symmetry test specimen texture third-order elastic constants Thurston and Brugger transducer transverse wave ultrasonic beam ultrasonic pulse uniaxial stress values wave along 100 wave normal wave speeds wave velocity Young's modulus