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Sec. 4–10 Limiters 265<br />

v out<br />

Ideal limiter<br />

characteristic<br />

v lim (t)<br />

V L<br />

V L<br />

v in<br />

V L<br />

t<br />

t<br />

v in (t)<br />

Figure 4–7<br />

Ideal limiter characteristic with illustrative input and unfiltered output waveforms.<br />

an ideal comparator with a zero reference level. The waveforms shown in Fig. 4–7 illustrate<br />

how amplitude variations in the input signal are eliminated in the output signal. A bandpass<br />

limiter is a nonlinear circuit with a saturating characteristic followed by a bandpass filter. In the<br />

case of an ideal bandpass limiter, the filter output waveform would be sinusoidal, since the<br />

harmonics of the square wave would be filtered out. In general, any bandpass input (even a<br />

modulated signal plus noise) can be represented, using Eq. (4–1b), by<br />

v in (t) = R(t) cos [v c t + u(t)]<br />

(4–54)<br />

where R(t) is the equivalent real envelope and u(t) is the equivalent phase function. The<br />

corresponding output of an ideal bandpass limiter becomes<br />

v out (t) = KV L cos [v c t + u(t)]<br />

(4–55)<br />

where K is the level of the fundamental component of the square wave, 4p, multiplied by the<br />

gain of the output (bandpass) filter. This equation indicates that any AM that was present on<br />

the limiter input does not appear on the limiter output, but that the phase function is preserved

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