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WAVES AND VIBRATIONS IN INHOMOGENEOUS STRUCTURES ...

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Relations to recent work 51<br />

Figure 5.9 Illustration of the compression of the pulse as it propagates through a spacetime<br />

optimized structure. From paper [21].<br />

these canbe partlyremoved if anexplicit penalizationterm is added to the objective<br />

function, although this generally causes the output pulse to deviate more from the<br />

target output.<br />

It turns out that if the two involved materials have different stiffness and mass<br />

density the possibility for manipulating the wave is greater. This however depends<br />

on the specific values of the parameters. An additional complication arises if the<br />

mass density varies in time. Then it becomes necessary to use a more sophisticated<br />

time-integration routine that is able to handle time-discontinuous velocity fields.<br />

Relations to recent work<br />

Optimization of dynamic systems in finite frequency ranges with Padé approximants<br />

was recently used by Donoso and Sigmund (2009). They considered the distribution<br />

of piezo-electric material in order to optimize the dynamic response of a mechanical<br />

structure.<br />

The system of non-linear oscillators studied in paper [19] has been further examined<br />

by Rothos and Vakakis (2009) who studied wave interaction in the case of<br />

essentially nonlinear oscillators. They did not consider optimization.

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