Abstract
The classical theory of wave propagation in elastic cylinders is extended to poro-elastic mandrel modes. The classical theory predicts the existence of undamped L modes and damped C, I, and Z modes. These waves also appear in poro-elastic mandrels, but all of them become damped because of viscous effects. The presence of the Biot slow bulk wave in the poro-elastic material is responsible for the generation of additional mandrel modes. One of them was already discussed by Feng and Johnson, and the others can be grouped together as so-called D modes. The damping of these D modes is at least as high as the damping of the free-field slow wave. [on SciFinder (R)]
| Original language | English |
|---|---|
| Pages (from-to) | 2049-2056 |
| Journal | Journal of the Acoustical Society of America |
| Volume | 122 |
| Issue number | 4 |
| DOIs | |
| Publication status | Published - 2007 |
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