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WAVES AND VIBRATIONS IN INHOMOGENEOUS STRUCTURES ...

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Phononic band-gap optimization<br />

-<br />

(a)<br />

TT11111111T<br />

I T I (b)<br />

!--II III I<br />

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(c)<br />

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Figure 10. Optimization of structure for minimum response at 2 = 63 kHz. (a) Structural<br />

domain and periodic boundary loading in the optimization procedure; (b) optimized topology;<br />

(c) average response at the right boundary when subjected to loading at the left boundary.<br />

Dashed line, a = 0, 3 = 50 x 103; solid line, a = = 0 0. High-contrast case.<br />

(corresponding to the centre frequency of the optimized gap of figure 7b). In order<br />

to obtain square symmetry of the resulting structure, we this time solve a multi-load<br />

problem. The structure is subjected to periodic excitation at the four edges independently,<br />

and we then minimize the sum of responses at the opposing edges. The<br />

optimization is performed with strong damping added (a = 0,/3 = 50 x 103) in order<br />

to remove resonance peaks and ensure stable convergence.<br />

Figure lOb shows the optimized structure. The topology is quasi-periodic and<br />

closely resembles the periodic band-gap structure in figure 4c. The largest difference<br />

between the two topologies is seen at the boundaries, where the finite structure<br />

has inclusions touching the boundaries and with a different periodicity. This prevents<br />

waves from propagating along the boundaries: a phenomenon that cannot be<br />

Phil. Trans. R. Soc. Lond. A (2003)<br />

1015<br />

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