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WAVES AND VIBRATIONS IN INHOMOGENEOUS STRUCTURES ...

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Topological material layout in plates for vibration suppression and wave propagation control<br />

Fig. 8 Topology and energy transport for the optimization problem<br />

sketched in Fig. 7. Only energy vectors larger than 10% of<br />

the maximum vector are shown<br />

wave device. The simply supported plate is excited by<br />

two harmonic forces, where one is phase shifted by a<br />

quarter of a period. This will initiate a wave in the<br />

plate. The objective function is defined as the energy<br />

through three groups of elements as sketched in Fig. 7.<br />

This example is inspired by the working principles of<br />

piezoelectric ring motors that rely on ring waves and<br />

friction between a stator and a rotor, see e.g. Uchino<br />

(1998).<br />

In Fig. 8 the optimized structure is shown along<br />

with the energy transport. We see that energy is being<br />

guided in a near-circular path as defined in the optimization<br />

problem but also that some energy escapes<br />

this path. This can for instance be seen in the lower right<br />

part of the plate. Especially at the lower optimization<br />

area we see that the energy vectors have a relatively<br />

large vertical component while in the other two areas<br />

the energy is more efficiently guided only in the desired<br />

direction.<br />

8 Conclusion<br />

We have presented a material layout algorithm based<br />

on the method of topology optimization. The algorithm<br />

allows for the design of bi-material elastic plates with<br />

optimized vibrational suppression and guided energy<br />

transport when subjected to harmonic excitation.<br />

The optimization algorithm is based on a finite element<br />

model of plate vibration for moderately thick<br />

plates using the Mindlin plate theory. Special consideration<br />

is given to the derivation of an energy transport<br />

measure using the Poynting vector.<br />

The optimization algorithm is based on the FE<br />

model combined with analytical sensitivity analysis performed<br />

with the adjoint method. An iterative optimization<br />

scheme is set up with design updates performed<br />

with the method of moving asymptotes.<br />

To demonstrate the capabilities of the method we<br />

have presented two sets of examples. The first deals<br />

with minimizing the total vibrational response of the<br />

plate in response to harmonic excitation at one or<br />

several distinct frequencies. The resulting bi-material<br />

designs display a low vibrational response at the target<br />

frequency range by moving the plate natural frequencies<br />

away from these targets.<br />

The second, and more challenging, set of examples<br />

deals with optimizing the materials distribution in order<br />

to direct the vibrational energy flow in specified paths<br />

in the plate. It was demonstrated that the specified<br />

energy transporting behavior could be realized by a<br />

complicated material layout and the rather difficult task<br />

of creating a ring wave device that functions by material<br />

contrasts was accomplished.<br />

Acknowledgements This work received support from the<br />

Eurohorcs/ESF European Young Investigator Award (www.esf.<br />

org/euryi) through the grant “Synthesis and topology optimization<br />

of optomechanical systems”, the New Energy and Industrial<br />

Technology Development Organization project (Japan), and<br />

from the Danish Center for Scientific Computing.<br />

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