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

### From inside the book

Results 1-3 of 31

Page 20

For the transverse waves a = 0, /?2 + y2 = 1 and El = y"^ . E2 = 0, £3 = 0, £T = El (

93) and consequently a = l, b = 0, c = 0 (94) and again the energy flows in the

same direction as the wave normal. Therefore in summary of

For the transverse waves a = 0, /?2 + y2 = 1 and El = y"^ . E2 = 0, £3 = 0, £T = El (

93) and consequently a = l, b = 0, c = 0 (94) and again the energy flows in the

same direction as the wave normal. Therefore in summary of

**plane wave**...Page 50

The strains produced in the test material by the propagating ultrasonic

extremely small and well within the linear ... To assure experimentally that the

these ...

The strains produced in the test material by the propagating ultrasonic

**wave**areextremely small and well within the linear ... To assure experimentally that the

**waves**used are indeed**plane**with little diffraction spread, we must generatethese ...

Page 114

On the other hand, as can be seen from our Eqs. (194), two transverse waves

propagating in the same direction do not interact with each other. Finally, he

noted that if two nonlinear

they will ...

On the other hand, as can be seen from our Eqs. (194), two transverse waves

propagating in the same direction do not interact with each other. Finally, he

noted that if two nonlinear

**plane waves**of either type intersect at an angle, thenthey will ...

### 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

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