Wave Manipulation by Topology Optimization - Solid Mechanics
Wave Manipulation by Topology Optimization - Solid Mechanics
Wave Manipulation by Topology Optimization - Solid Mechanics
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Chapter 3<br />
<strong>Topology</strong> optimization of wave problems<br />
As briefly mentioned in the previous chapter the spatial placement and distribution<br />
of the material properties determines how a wave behaves in a medium. Control<br />
of these material properties allows us to manipulate wave propagation for various<br />
purposes. The material as well as material layout needed in wave devices like Bragg<br />
gratings[15], invisibility cloaks[16] and Fresnel zone plate lenses[17] can be derived<br />
directly <strong>by</strong> analytic means. Such applications were developed <strong>by</strong> ingenious physicists<br />
with great physical insight. However, in some cases the derived material properties<br />
are very challenging to realize especially in the optical regime (e.g. invisibility<br />
cloaks[16]), and in other cases the geometrical layout rule is known not to be optimal<br />
(e.g. Fresnel zone plate lenses[18]). <strong>Optimization</strong> methods may be used as an<br />
efficient design tool for such problems. <strong>Topology</strong> optimization is a gradient based<br />
optimization method that work <strong>by</strong> varying the distribution of materials within a<br />
bounded design domain. The strength of this method is that it can change the<br />
shape topology without any geometrical constraints on the design. Originally the<br />
method was developed <strong>by</strong> Kikuchi and Bendsøe using a homogenization technique<br />
to minimize the compliance of continuum structures[19]. Since then the method<br />
has been extended to other fields of engineering such as heat transfer (e.g. [20]),<br />
fluid dynamics (e.g. [21]), micro electro-mechanical systems (e.g. [22, 23]), photonics<br />
(e.g. [24, 25]) and acoustics (e.g. [6]). Today implementations[26, 27] of the topology<br />
optimization method for structural problems are available free of charge intended<br />
for educational purposes and even commercial software packages such as OptiStruct<br />
<strong>by</strong> Altair and TOSCA <strong>by</strong> FE-Design exist. The purpose of this chapter is to give<br />
a brief introduction to topology optimization and how it is applied to the acoustic<br />
and electromagnetic wave manipulation problems covered in this thesis. A thorough<br />
description of the topology optimization method can be found in the monograph <strong>by</strong><br />
Bendsøe and Sigmund[28].<br />
3.1 <strong>Topology</strong> optimization of acoustic and electromagnetic<br />
wave propagation problems<br />
The behavior of electromagnetic waves is determined <strong>by</strong> the distribution of dielectric<br />
material, magnetic material, air and/or metal. The first material distribution<br />
technique concerning electromagnetic waves was reported more than a decade<br />
ago[29, 30]. In the study, dielectric material was distributed in order to maximize<br />
the band gap in 2D photonic crystals. Not long after the initial study, the transmission<br />
through photonic crystal wave guide bends[24] and splitters[31] was maximized<br />
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