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THESE de DOCTORAT - cerfacs

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4.1 Fundamental validation cases 59<br />

e 2<br />

r i<br />

x<br />

dV i<br />

r j<br />

y i<br />

y j<br />

e 1<br />

dV j<br />

Figure 4.1: Monopoles placed at y and listener placed at x<br />

where k = ω/ ¯c 2 and Ŝ(y, ω) is a forcing source term. In this equation y represents the distance<br />

from the source to the reference point and x represents the distance from the observer to the<br />

reference point as illustrated in Fig. 4.1. The solution of this equation can be found by applying<br />

Eq. (2.74)<br />

ˆp(x, ω) =<br />

∫<br />

V 0 (y)<br />

Ŝ(y, ω)<br />

¯c 2 Ĝ(x|y, ω)dy (4.2)<br />

The 2D spectral Green’s function, given by Eq. (2.82), is inserted into Eq. (4.2) resulting in<br />

ˆp(x, ω) =<br />

i<br />

4¯c 2<br />

∫<br />

V 0 (y)<br />

Ŝ(y, ω)H 2 0(kr)dy (4.3)<br />

where r = |x − y| and H0 2 is the Hankel function of the second kind and or<strong>de</strong>r 0.<br />

4.1.1 A Monopole in free space<br />

One fundamental validation for an acoustic co<strong>de</strong> is to test its ability to compute the radiation of<br />

sound due to a source. As a consequence, for the present case only one monopole is consi<strong>de</strong>red<br />

and no boundary conditions are taken into account. Moreover, as mentioned before, the mean<br />

field is consi<strong>de</strong>red homogeneous. These conditions are imposed so that a perfect isotropic<br />

radiation pattern is obtained. The source is pointwise and is <strong>de</strong>fined as

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