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Problems 307<br />

where m(t) is the modulating signal and v c = 2pf c , in which f c is the carrier frequency. Show that<br />

the functions g(t), x(t), y(t), R(t), and u(t), as given for FM in Table 4–1, are correct.<br />

4–13 The output of a FM transmitter at 96.9 MHz delivers 25kw average power into an antenna system<br />

which presents a 50-Ω resistive load. Find the value for the peak voltage at the input to the<br />

antenna system.<br />

★ 4–14 Let a modulated signal,<br />

s(t) = 100 sin(v c + v a )t + 500 cos v c t - 100 sin (v c - v a )t<br />

where the unmodulated carrier is 500 cos v c t.<br />

(a) Find the complex envelope for the modulated signal. What type of modulation is involved?<br />

What is the modulating signal?<br />

(b) Find the quadrature modulation components x(t) and y(t) for this modulated signal.<br />

(c) Find the magnitude and PM components R(t) and u (t) for this modulated signal.<br />

(d) Find the total average power, where s(t) is a voltage waveform that is applied across a 50-Ω<br />

load.<br />

★ 4–15 Find the spectrum of the modulated signal given in Prob. 4–14 by two methods:<br />

(a) By direct evaluation using the Fourier transform of s(t).<br />

(b) By the use of Eq. (4–12).<br />

4–16 Given a pulse-modulated signal of the form<br />

s(t) = e -at cos [1v c +¢v2t]u(t)<br />

where a, v c , and ∆v are positive constants and the carrier frequency, w c ¢v,<br />

(a) Find the complex envelope.<br />

(b) Find the spectrum S( f ).<br />

(c) Sketch the magnitude and phase spectra |S( f)| and u(f) = lS(f) .<br />

4–17 In a digital computer simulation of a bandpass filter, the complex envelope of the impulse<br />

response is used, where h(t) = Re[k(t) e jvct ], as shown in Fig. 4–3. The complex impulse<br />

response can be expressed in terms of quadrature components as k(t) = 2h x (t) + j2h y (t),<br />

where h x(t) = 1 and h y (t) = 1 2<br />

Im [k(t)].<br />

2 Re[k(t)] The complex envelopes of the input and<br />

output are denoted, respectively, by g 1 (t) = x 1 (t) + jy 1 (t) and g 2 (t) = x 2 (t) + jy 2 (t). The bandpass<br />

filter simulation can be carried out by using four real baseband filters (i.e., filters having real<br />

impulse responses), as shown in Fig. P4–17. Note that although there are four filters, there are<br />

only two different impulse responses: h x (t) and h y (t).<br />

(a) Using Eq. (4–22), show that Fig. P4–17 is correct.<br />

(b) Show that h y (t) K 0 (i.e., no filter is needed) if the bandpass filter has a transfer function with<br />

Hermitian symmetry about f c —that is, if H(-∆f + f c ) = H ✽ (∆f + f c ), where |∆ f | 6 B T 2 and B T<br />

is the bounded spectral bandwidth of the bandpass filter. This Hermitian symmetry implies<br />

that the magnitude frequency response of the bandpass filter is even about f c and the phase<br />

response is odd about f c .<br />

4–18 Evaluate and sketch the magnitude transfer function for (a) Butterworth, (b) Chebyshev, and<br />

(c) Bessel low-pass filters. Assume that f b = 10 Hz and P = 1.<br />

★ 4–19 Plot the amplitude response, the phase response, and the phase delay as a function of frequency<br />

for the following low-pass filters, where B = 100 Hz:

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