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Sec. 4–4 Evaluation of Power 247<br />

where, because m(t) is real, M*( f ) = M(-f ) and d ( f ) = d (-f ) (the delta function was defined to be<br />

even) were used. Suppose that the magnitude spectrum of the modulation happens to be a triangular<br />

function, as shown in Fig. 4–2a. This spectrum might arise from an analog audio source in which<br />

the bass frequencies are emphasized. The resulting AM spectrum, using Eq. (4–20a), is shown in<br />

Fig. 4–2b. Note that because G(f - f c ) and G * (-f - f c ) do not overlap, the magnitude spectrum is<br />

ƒ S(f) ƒ = e<br />

1<br />

2 A cd(f-f c ) + 1 2 A c |M(f-f c )|, f 7 0<br />

1<br />

2 A cd(f+f c ) + 1 2 A c |M(-f-f c )|, f 6 0<br />

(4–20b)<br />

The 1 in g(t) = A c [1 + m(t)] causes delta functions to occur in the spectrum at f = ; f c , where f c<br />

is the assigned carrier frequency. Using Eq. (4–17), we obtain the total average signal power<br />

P s = 1 2 A c 2 8|1 + m(t)| 2 9 = 1 2 A c 2 81 + 2m(t) + m 2 (t)9<br />

= 1 2 A c 2 [1 + 28m(t)9 + 8m 2 (t)9]<br />

If we assume that the DC value of the modulation is zero, as shown in Fig. 4–2a, the average signal<br />

power becomes<br />

P s = 1 2 A c 2 [1 + P m ]<br />

(4–21)<br />

1<br />

2 A c 2<br />

where P is the power in the modulation m(t), is the carrier power, and 2 A c 2 m = 8m 2 (t)9<br />

P m is<br />

the power in the sidebands of s(t).<br />

1<br />

|M(f)|<br />

1.0<br />

–B B<br />

f<br />

(a) Magnitude Spectrum of Modulation<br />

1<br />

2<br />

|S(f)|<br />

Discrete carrier term<br />

1<br />

with weight = – A<br />

2 c<br />

Weight = – A c<br />

A c<br />

Lower<br />

2<br />

sideband<br />

Upper<br />

sideband<br />

–f c -B – f c –f c +B f c -B f c f c +B<br />

(b) Magnitude Spectrum of AM Signal<br />

Figure 4–2<br />

Spectrum of AM signal.<br />

f

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