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WAVES AND VIBRATIONS IN INHOMOGENEOUS STRUCTURES ...

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ρ=1<br />

κ=1<br />

1<br />

R<br />

Figure 1 - A one-dimensional acoustic wave in air is partially reflected (R) and transmitted (T )<br />

at the interface to an acoustic medium.<br />

and define continuous property interpolation functions ρ(̺) and κ(̺) that fulfill the<br />

following conditions:<br />

<br />

1, ̺ = 0<br />

1, ̺ = 0<br />

ρ(̺) =<br />

ρ2<br />

ρ1<br />

T<br />

, ̺ = 1 , κ(̺) =<br />

ρ<br />

κ<br />

κ2,<br />

̺ = 1 κ1<br />

The introduction of continuous properties allows us to compute the gradients of the<br />

objective functional with respect to the indicator function: dΦ/d̺, and we can thus use<br />

a gradient based optimization strategy with ̺ as a topological design variable.<br />

Clearly, we are only interested in binary values (0 or 1) of the indicator function<br />

in our optimized design, and our optimization formulation must include a strategy to<br />

avoid intermediate values of ̺ in the final design. Various strategies exist to ensure a<br />

binary design (see e.g. [5]) and in this work we rely on the choice of the functions ρ(̺)<br />

and κ(̺). To find suitable candidates we study a simple 1D acoustic system (Fig. 1).<br />

A unit magnitude wave propagating in air is partially transmitted (T ) and partially<br />

reflected (R) at the interface to an acoustic medium with the material properties ρ(̺)<br />

and κ(̺). The amplitudes of the reflected and the transmitted wave are:<br />

R =<br />

√ κρ − 1<br />

√ κρ + 1 , T =<br />

(4)<br />

2<br />

√ κρ + 1 , (5)<br />

so that R → 1, T → 0 when κρ → ∞ (a perfectly rigid solid), and R = 0, T = 1<br />

when κρ = 1 (air).<br />

We want to choose our interpolation functions so that the reflection from the<br />

acoustic medium is a smooth and well-behaved function of ̺. One possible choice is<br />

the polynomial form:<br />

ρ(̺) = 1 + ̺ q1<br />

ρ2<br />

( − 1), κ(̺) = 1 + ̺ q2<br />

κ2<br />

( − 1). (6)<br />

ρ1<br />

The reflection versus ̺ is depicted in Fig. 2(left) for different values of q1 and q2<br />

(ρ2/ρ1 = κ2/κ1 = 500). All curves have vanishing slope at ̺ = 1, which turns<br />

out to make it difficult to obtain well defined solid regions in the design.<br />

Instead, inspired by the Helmholtz equation, we use polynomial interpolation in<br />

ρ −1 and κ −1 :<br />

ρ(̺) −1 = 1 + ̺ q1<br />

ρ2<br />

(( ) −1 − 1), κ(̺) −1 = 1 + ̺ q1<br />

κ2<br />

(( ) −1 − 1). (7)<br />

ρ1<br />

3<br />

κ1<br />

κ1

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