Notes on Acoustics

Appendix A: Supplementary Notes

A.1 Fourier Series and Spectra

A.1.1 Fourier Transform. Spectrum of Finite Harmonic Wave Train

Consider an oscillation of finite length, a chirp, such that F(t) = A cos( ? 0 t) between t = ? t 0 and t = t 0 and zero elsewhere. According to Eq. 2.67, the Fourier amplitude of this function is


where ? = 2 ?? and X + = ( ? + ? 0) t 0 and X ? = ( ? ? ? 0) t 0, which, for computational purposes, we express as X = ( ? 1)2 ?t 0 /T 0, where T 0 = 2 ?/ ? 0 is the period and ? = ?/ ? 0. With reference to Section 2.6.3, the energy spectrum density is E( ?) = 2 F( ?) 2 and it should be recalled that only positive frequencies are involved in this expression. In Fig. A.1 are shown the energy spectra for signal lengths from 0.5 to 8 periods. The 0.5 period signal covers the central maximum of the signal and, unlike the other cases, has a time average different from zero. This is the reason why the corresponding spectrum is quite different from the others; it has a maximum at zero frequency. Such a pulse is typical for explosive events which are...

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