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Getting to Grips with Aircraft Noise

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Flight Operations Support & Line Assistance<br />

<strong>Getting</strong> <strong>to</strong> grips <strong>with</strong> aircraft noise<br />

9 - A BIT OF THEORY<br />

• More generally, any periodic sound signal can be split up in<strong>to</strong> FOURIER series<br />

(decomposition as the infinite sum of elementary pure sounds)<br />

∑ ∞<br />

p t)<br />

C n<br />

( = sin ( nωωωωt<br />

+ ϕϕϕϕ )<br />

0<br />

where : ωωωω corresponds <strong>to</strong> the fundamental pulsation<br />

nωωωω are the harmonics.<br />

Cn are the Fourier coefficients (amplitude of each elementary<br />

pure <strong>to</strong>ne)<br />

C n<br />

Fundamental<br />

• Practically, a sound is not periodic and thus cannot be split up in<strong>to</strong> a Fourier<br />

series. In that case, the frequency spectrum is continuous and the previously<br />

mentioned Fourier series become an integral called the Fourier transform.<br />

Then, any sound can be expressed thanks <strong>to</strong> the inverse Fourier transform<br />

(C(f) being the direct Fourier transform of p(t)), which makes the pair <strong>with</strong> the<br />

Fourier series when the signal period becomes infinite.<br />

∫ +∞<br />

−∞<br />

f 0 2f 0 3f 0 …<br />

jωt<br />

p(<br />

t)<br />

= C(<br />

f ) e df<br />

Harmonics<br />

Where: C(f) is called spectrum of the acoustic pressure p(t).<br />

f<br />

65

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