Abstract
We show that the frequency spectrum of two-component elastic laminates admits a universal structure, independent of the geometry of the periodic-cell and the specific physical properties. The compactness of the structure enables us to rigorously derive the maximal width, the expected width, and the density of the band-gaps - ranges of frequencies at which waves cannot propagate. In particular, we find that the density of these band-gaps is a universal property of classes of laminates. Rules for tailoring laminates according to desired spectrum properties thereby follow. We show that the frequency spectrum of various finitely deformed laminates are also endowed with the same compact structure. Finally, we explain how our results generalize for laminates with an arbitrary number of components, based on the form of their dispersion relation.
Original language | English |
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Pages (from-to) | 127-136 |
Number of pages | 10 |
Journal | Journal of the Mechanics and Physics of Solids |
Volume | 92 |
DOIs | |
State | Published - 1 Jul 2016 |
Externally published | Yes |
Keywords
- Band-gap
- Bloch-Floquet waves
- Dispersion relation
- Finite deformations
- Frequency spectrum
- Laminate
- Phononic crystal
- Wave propagation
ASJC Scopus subject areas
- Condensed Matter Physics
- Mechanics of Materials
- Mechanical Engineering