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THESE de DOCTORAT - cerfacs

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4.1 Fundamental validation cases 61<br />

150<br />

210<br />

120<br />

240<br />

90<br />

270<br />

0.008<br />

60<br />

0.006<br />

0.004<br />

0.002<br />

180 0<br />

300<br />

30<br />

330<br />

r = 0.05<br />

r = 0.15<br />

Pressure Fluctuation (Pa)<br />

0.03<br />

0.02<br />

0.01<br />

0<br />

−0.01<br />

−0.02<br />

Analytics<br />

AVSP−f<br />

−0.03<br />

−0.2 −0.1 0 0.1 0.2<br />

X axis (m)<br />

a) | ˆp| Directivity of a monopole b) Pressure fluctuation<br />

for two different radii.<br />

along the horizontal e 1 axis<br />

[ —— Analytics, (◦△) AVSP-f ] [ —— Analytics, (◦) AVSP-f ]<br />

Figure 4.4: Analytical solution vs Numerical solution.<br />

4.1.2 A Dipole in free space<br />

Once pure radiation is tested in section (4.1.1), the influence on the acoustic field of another<br />

monopole is tested. If this monopole radiates sound out of phase with respect to the first<br />

monopole, a substraction of acoustic fluctuations will occur leading to a diminution of the<br />

acoustic amplitu<strong>de</strong> in some regions. If this phase shift is equal to π a perfect cancelation should<br />

occur in the plane of antisymmetry between the two monopoles. Two monopoles with such a<br />

shift phase conform a dipole. The source is <strong>de</strong>fined as<br />

Ŝ(y, ω) = Ŝ 0 δ(y − y 1 )e −iφ 1<br />

+ Ŝ 0 δ(y − y 2 )e −iφ 2<br />

(4.5)<br />

where φ 1 = φ 2 + π. From Eq. (4.3)<br />

ˆp(x, ω) =<br />

i ∫<br />

4c 2 0<br />

V 0 (y)<br />

(Ŝ0 δ(y − y 1 )e −iφ 1<br />

+ Ŝ 0 δ(y − y 2 )e 2)<br />

−iφ H0(kr)dV 2 (4.6)<br />

Finally<br />

ˆp(x, ω) =<br />

i (Ŝ0 δ(y − y 1 )e 1)<br />

−iφ H0(kr 2 1 )dV 1 +<br />

4c 2 0<br />

i<br />

4c 2 0<br />

(Ŝ0 δ(y − y 2 )e 2)<br />

−iφ H0(kr 2 2 )dV 2 (4.7)

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