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WAVES AND VIBRATIONS IN INHOMOGENEOUS STRUCTURES ...

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18 Chapter 3 Bandgap structures as optimal designs<br />

In paper [8] the optimization problem is extended to the case of transverse vibrations<br />

and waves in moderately thick plates. The paper deals with optimizing the<br />

distribution of two elastic materials in order to suppress forced vibrations or guide<br />

elastic waves in designated paths in the plate.<br />

Paper [9] studies a closely related problem in a quite different physical setting.<br />

Solid material is distributed in an acoustic chamber in order to minimize the transmission<br />

of acoustic waves throughthe chamber. The problem isconsidered for waves<br />

in a finite frequency range.<br />

Main references<br />

The design of phononic bandgap structures using a material distribution optimization<br />

method is believed to be a novel contribution of this thesis. Topology optimization<br />

methods had previously been used to design structures subjected to forced<br />

vibrations in the lower frequency range by Ma et al. (1993) for 2D elastic problems<br />

and by Soto and Diaz (1993) for plate structures. Tcherniak (2002) considered optimization<br />

of resonating structures and Jog (2002) optimized plates for minimum<br />

dynamic compliance by considering the dissipated energy. Optimization problems<br />

related to maximization and minimization of eigenfrequencies had also been considered<br />

using topology optimization, e.g. by Diaz and Kikuchi (1992) for 2D elastic<br />

structures and by Pedersen (2000) for plates. Ma et al. (1994) and Osher and Santosa<br />

(2001) considered the problem of separating eigenfrequencies. However, here<br />

the separation of low order eigenfrequencies was examined with no special consideration<br />

to bandgap structures.<br />

Topology optimization of plate structures for maximum bandgaps was first explored<br />

by the author, Ole Sigmund and Søren Halkjær (Halkjær et al., 2006). Diaz<br />

et al. (2005) had previously studied maximization of bandgaps in similar beam grillage<br />

structures.<br />

The problem of using topology optimization to design acoustic structures was<br />

proposed in two conference papers by the author, Ole Sigmund and co-workers<br />

(Sigmund and Jensen, 2003; Sigmund et al., 2004).<br />

3.1 Vibration-quenching structures<br />

The primary optimization problem is:<br />

What is the optimal distribution of two elastic materials in a structure<br />

so that the forced vibration response is minimized?<br />

Fig.3.1ashowsthemodelusedtocreatetheoptimizedstructures. Afreeplanartwodimensional<br />

structure (plane-strain condition) is subjected to forced vibrations by a<br />

harmonicload(withfrequency Ω) actingalongafreeedge. Thevibrationresponse is<br />

minimized alongtheoppositeedge. Fig.3.1billustratestheoptimizeddistributionof

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