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B. P. Lathi, Zhi Ding - Modern Digital and Analog Communication Systems-Oxford University Press (2009)

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174 AMPLITUDE MODULATIONS AND DEMODULATIONS

Figure 4.26

Phase-locked

loop and its

equivalent

circuit.

A sin fw c t + om]

Loop

filter

H(s)

Voltagecontrolled

oscillator

eo(t)

(a)

0;(1) sin( ) AKH(s)

8 0 = ce 0 (t)

0/t)

r 0

(b)

Basic PLL Operation

The operation of the PLL is similar to that of a feedback system (Fig. 4.26a). In a typical

feedback system, the feedback signal tends to follow the input signal. If the feedback signal

is not equal to the input signal, the difference (known as the error) will change the feedback

signal until it is close to the input signal. A PLL operates on a similar principle, except that the

quantity fed back and compared is not the amplitude, but the phase. The VCO adjusts its own

frequency such that its frequency and phase can track those of the input signal. At this point,

the two signals are in synchronism (except for a possible difference of a constant phase).

The voltage-controlled oscillator (VCO) is an oscillator whose frequency can be linearly

controlled by an input voltage. If a VCO input voltage is e 0 (t), its output is a sinusoid with

instantaneous frequency given by

w(t) = W e + ce 0 (t) (4.30)

where c is a constant of the VCO and W e is the free-running frequency of the VCO [ when

e 0 (t) = O]. The multiplier output is further low-pass-filtered by the loop filter and then applied

to the input of the VCO. This voltage changes the frequency of the oscillator and keeps the

loop locked by forcing the VCO output to track the phase (and hence the frequency) of the

input sinusoid.

If the VCO output is B cos [w e t+ 0 0 (t)], then its instantaneous frequency is W e + 0 0 (t).

Therefore,

(4.31)

Note that c and B are constant parameters of the PLL.

Let the incoming signal (input to the PLL) be A sin [w e t + 0i (t)]. If the incoming signal

happens to be A sin [w 0 t + i,{!(t)], it can still be expressed as A sin [w e t+ 0; (t)], where 0;(t) =

(w 0 - w c )t + i,/J(t). Hence, the analysis that follows is general and not restricted to equal

frequencies of the incoming signal and the free-running VCO signal.

The multiplier output is

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