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120<br />

w(t)<br />

Signals and Spectra Chap. 2<br />

4<br />

3<br />

2<br />

1<br />

–4 –3 –2 –1 1 2 3 4<br />

t<br />

Figure P2–19<br />

(c) x(t) = 2 dw(t) .<br />

dt<br />

(d) x(t) = w(1 - t).<br />

2–21 From Eq. (2–30), find w(t) for W(f) = Aß(f/2B), and verify your answer by using the duality<br />

property.<br />

2–22 Find the quadrature spectral functions X(f) and Y(f) for the damped sinusoidal waveform<br />

w(t) = u(t)e -at sin v 0 t<br />

where u(t) is a unit step function, a 7 0, and W(f) = X(f) + jY(f).<br />

2–23 Derive the spectrum of w(t) = e -|t|/T .<br />

★ 2–24 Find the Fourier transforms for the following waveforms. Plot the waveforrns and their magnitude<br />

spectra. [Hint: Use Eq. (2–184).]<br />

(a) ßa t - 3 b.<br />

4<br />

(b) 2.<br />

(c) a t - 5 b.<br />

5<br />

2–25 By using Eq. (2–184), find the approximate Fourier transform for the following waveform:<br />

sin(2pt/512) + sin(70pt512), 5 6 t 6 75<br />

x(t) = e<br />

0, t elsewhere<br />

2–26 Evaluate the spectrum for the trapezoidal pulse shown in Fig. P2–26.<br />

2–27 Show that<br />

-1 {[w(t)]} = w(t)<br />

[Hint: Use Eq. (2–33).]<br />

2–28 Using the definition of the inverse Fourier transform, show that the value of w(t) at t = 0 is equal<br />

to the area under W(f). That is, show that<br />

q<br />

w(0) = W(f) df<br />

L<br />

-q

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