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540<br />

Performance of Communication Systems Corrupted by Noise Chap. 7<br />

The output SNR can also be expressed in terms of the equivalent baseband system by substituting<br />

Eq. (7–84) into Eq. (7–115), where P s = A 2 c >2:<br />

(S>N) out<br />

= b 2 (7–120)<br />

(S>N) p a m 2<br />

b<br />

baseband V p<br />

This equation shows that the improvement of a PM system over a baseband signaling<br />

system depends on the amount of phase deviation that is used. It seems to indicate that we can<br />

make the improvement as large as we wish simply by increasing b p . This depends on the types<br />

of circuits used. If the peak phase deviation exceeds p radians, special “phase unwrapping”<br />

techniques have to be used in some circuits to obtain the true value (as compared with the<br />

relative value) of the phase at the output. Thus, the maximum value of b p m(t)/V p = D p m(t)<br />

might be taken to be p. For sinusoidal modulation, this would provide an improvement of<br />

D 2 p m 2 = p 2 >2, or 6.9 dB, over baseband signaling.<br />

It is emphasized that the results obtained previously for (S/N) out are valid only when the<br />

input signal is above the threshold [i.e., when (SN) in 7 1].<br />

FM Systems<br />

The procedure that we will use to evaluate the output SNR for FM systems is essentially the<br />

same as that used for PM systems, except that the output of the FM detector is proportional to<br />

du T (t)/dt, whereas the output of the PM detector is proportional to u T (t). The detector in the<br />

angle modulated receiver of Fig. 7–21 is now an FM detector. The complex envelope of the<br />

FM signal (only) is<br />

where<br />

g s (t) = A c e ju s(t)<br />

t<br />

u s (t) = D f m(l) dl<br />

L<br />

(7–121a)<br />

(7–121b)<br />

It is assumed that an FM signal plus white noise is present at the receiver input.<br />

The output of the FM detector is proportional to the derivative of the composite phase at<br />

the detector input:<br />

r 0 (t) = a K (7–122)<br />

2p b d lgT(t)<br />

= a K dt 2p b du T (t)<br />

dt<br />

In this equation, K is the FM detector gain. Using the same procedure as that leading to<br />

Eqs. (7–108), (7–110), and (7–111), we can approximate the detector output by<br />

-q<br />

r 0 (t) L s 0 (t) + n 0 (t)<br />

(7–123)<br />

where, for FM,<br />

and<br />

s 0 (t) = a K 2p b du s (t)<br />

dt<br />

= a KD f<br />

2p b m(t)<br />

(7–124a)

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