Abstract

Pentamode materials are artificial solids with elastic properties that approximate those of isotropic liquids. The corresponding three-dimensional mechanical metamaterials or ‘meta-liquids’ have recently been fabricated. In contrast to normal liquids, anisotropic meta-liquids are also possible—a prerequisite for realizing many of the envisioned transformation-elastodynamics architectures. Here, we study several possibilities theoretically for introducing intentional anisotropy into three-dimensional pentamode metamaterials. In static continuum mechanics, the transition from anti-auxetic pentamode materials to auxetics is possible. Near this transition, in the dynamic case, approximately uniaxial versions of pentamode metamaterials deliver anisotropic longitudinal-wave phase velocities different by nearly a factor of 10 for realistically accessible microstructure parameters.

Highlights

  • Panels (b) and (c) illustrate two examples of anisotropic versions of pentamode metamaterials in which P has been moved along the space diagonal. (b) p =

  • This shifting leads to a reduced crystal symmetry and to more anisotropic wave propagation

  • At p = 33.3%, we find extrema for both red velocities versus the position of the point P, indicating a special mechanical behavior or a transition at this geometrically special point

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Summary

Introduction

It is clear from the geometry that one can expect a different wave velocity for propagation along the fcc cube’s space diagonal than for directions perpendicular to that axis. For the geometrical structure parameters, we choose the small diameter d = 0.55 μm (see figure 1(a)), the large diameter D = 3 μm and an fcc extended unit cell lattice constant of a constant corresponds Panels (a)–(c) of figure 2 depict calculated band structures for different positions of P on the fcc cube’s space diagonal.

Results
Conclusion
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