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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4.4 Effect of polarization and background material[P2] 25<br />
<br />
<br />
Figure 4.4 The cloak (a) for 1 symmetry line is near perfect at 0 o (b) whereas significant<br />
scattering is generated at 5 o (c) The dielectric layout (e) for the cloak optimized to operate<br />
in an interval from -5 o to 5 o are effective both for incident angles of 0 o (f) and 5 o (g). The<br />
robust design for small variation in the angle of incidence comes at the cost of increased<br />
scattering (d).<br />
make the cloak more versatile to various angles of incidence, more symmetry lines<br />
are added to the design domain at the cost of increased objective value.<br />
As mentioned above a slight variation in the incident angle results in a deteriorated<br />
cloaking performance. The cloak for 1 symmetry line is near perfect at<br />
0 o whereas significant scattering is generated at 5 o as shown in figures 4.4(b) and<br />
(c). A robust design for small perturbations in the angle of incidence is obtained<br />
<strong>by</strong> illuminating with uniform waves incident in an interval from -5 o to 5 o on the<br />
design domain and cylinder. The optimization is formulated as a min/max problem,<br />
i.e. the load case, which yields the highest scattering in each iteration step is<br />
minimized. The angle sweep in figure 4.4(d) and the fields patterns in figures 4.4(f)<br />
and (g) clearly shows that the cloak from figure 4.4(e) can be operated in a broader<br />
incident angle interval at the cost of increased scattering.<br />
4.4 Effect of polarization and background material[P2]<br />
Finishing the initial study we wanted to pursue a realization of an all-dielectric fully<br />
enclosing optical cloak designed <strong>by</strong> topology optimization. In a possible future experimental<br />
setup it may be easier to confine the polarized propagating wave in a<br />
material with higher index than free space and let spatial distributed areas of free<br />
space constitute the optimized design profile of the cloak. This is the ”inverse”<br />
case of the previous study, which was based on distributing material with a higher<br />
permittivity than the background material (free space). Intuitively, distributing dielectric<br />
material having a lower permittivity than the background material would<br />
result in cloaking performance on the same level or better, however, this is not the