Relation Between Spectral Width and Coherence Time. Show that the coherence time T. defined in (12.1-10) is related to the spectral width Av, defined in (12.1-18) by the simple inverse relation T. = 1/Avc. Hint: Use the definitions of Ave and Te, the Fourier-transform relation between S(v) and G(t), and Parseval’s theorem provided in (A.1-7) [Appendix A].

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Relation Between Spectral Width and Coherence Time. Show that the coherence time 7.
defined in (12.1-10) is related to the spectral width Ave defined in (12.1-18) by the simple inverse
relation T. = 1/Ave. Hint: Use the definitions of Av, and Te, the Fourier-transform relation between
S(v) and G(7), and Parseval's theorem provided in (A.1-7) [Appendix A].
Te =
dr
(12.1-10)
Coherence Time
2
S(v).
Ave
(12.1-18)
| s°(v) dv
• Parseval's Theorem. The signal energy, which is the integral of the signal power
|f(t)l², equals the integral of the energy spectral density [F(v)l², so that
IS)P dt =
\F(w)F dv.
(A.1-7)
Parseval's Theorem
Transcribed Image Text:Relation Between Spectral Width and Coherence Time. Show that the coherence time 7. defined in (12.1-10) is related to the spectral width Ave defined in (12.1-18) by the simple inverse relation T. = 1/Ave. Hint: Use the definitions of Av, and Te, the Fourier-transform relation between S(v) and G(7), and Parseval's theorem provided in (A.1-7) [Appendix A]. Te = dr (12.1-10) Coherence Time 2 S(v). Ave (12.1-18) | s°(v) dv • Parseval's Theorem. The signal energy, which is the integral of the signal power |f(t)l², equals the integral of the energy spectral density [F(v)l², so that IS)P dt = \F(w)F dv. (A.1-7) Parseval's Theorem
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