Partial Differential Equations - Modelling and ... - ResearchGate
Partial Differential Equations - Modelling and ... - ResearchGate
Partial Differential Equations - Modelling and ... - ResearchGate
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108 I. Sazonov et al.<br />
6.4 Scattering by a PEC NACA0012 Aerofoil<br />
The next example involves the simulation of scattering of a plane single frequency<br />
wave, directed along the x-axis, by a perfectly conducting NACA0012<br />
aerofoil of length λ. The aim of this example is to analyse the performance<br />
of the numerical schemes when the geometry exhibits high curvature. A<br />
benchmark solution is computed using an unstructured mesh with spacing<br />
λ/120. The unstructured mesh is generated, outside the aerofoil, in the region<br />
−λ ≤ x, y ≤ λ. The scattering width distributions computed on this<br />
mesh with the co-volume scheme <strong>and</strong> the FETD scheme proved to be identical.<br />
An unstructured mesh was generated to meet the spacing requirement<br />
of λ/15. Another unstructured mesh, providing better representation of the<br />
leading edge curvature, is generated by locally reducing the mesh spacing in<br />
the vicinity of the leading edge of the airfoil by a factor of 2. A view of both<br />
these meshes is shown in Figure 11.<br />
The computed scattering width distributions are compared with the benchmark<br />
distribution in Figure 12. It can be observed that the co-volume results<br />
are better on the uniform mesh <strong>and</strong> that the accuracy of the FETD results improve<br />
with the local refinement in the leading edge region. For this example,<br />
Table 4 shows the values of spc, time <strong>and</strong> E SW . The co-volume method is<br />
approximately 30 times faster than FETD for this example.<br />
6.5 Scattering by a PEC Cavity<br />
The final example considers the simulation of scattering of a plane single<br />
frequency wave by a U-shaped PEC cavity. The thickness of the cavity walls<br />
is equal to 0.4λ, the internal cavity width is 2λ <strong>and</strong> the internal cavity length<br />
is 8λ. In the simulation, the wave is incident upon the open end of the cavity<br />
<strong>and</strong> propagates in a direction which lies at an angle θ =30 ◦ to the main<br />
axis of the cavity. An unstructured mesh is employed, with typical spacing<br />
λ/15, in the region that lies within a distance of λ from the scatterer, as<br />
(a)<br />
(b)<br />
Fig. 11. Details of the unstructured meshes employed for the simulation of scattering<br />
of a plane TE wave by a PEC NACA0012 aerofoil of length λ showing (a) the<br />
uniform mesh, (b) the locally refined mesh.