THESE de DOCTORAT - cerfacs
THESE de DOCTORAT - cerfacs
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