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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.

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