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PHASE LOCKED LOOP APPLICATIONSThe natural frequency (w n ) of a loop in its final circuitconfiguration can be measured by applying a frequencymodulated signal of the desired amplitude to the loop(Table 8-2 shows that the natural frequency is a functionof Kd, in turn a function of input amplitude). As themodulation frequency (w m ) is increased, the phaserelationship between the modulation and recovered sinewave will go through 90 0 at Sm = wn and the outputamplitude will peak.UNDERDAMPED ~ ~ 0.3DAMPING (nAs shown in Table 8-2 in the discussion on low pass filter,damping is a function of Ko, Kd and the low pass filter.Since Ko and Kd are functions of center frequency andinput amplitude, respectively, damping is highly dependenton the particular operating condition of the loop. Dampingestimates for the desired operating condition can be madeby applying an input signal which is frequency modulatedwithin the lock range by a square wave. The low pass filtervoltage is then monitored on an oscilloscope which issynchronized to the modulating waveform, as shown inFigure 8-16. Figure 8-17 shows typical waveformsdisplayed. The loop damping can be estimated by comparingthe number and magnitude of the overshoots withthe graph of Figure 8-18, which gives the transient phaseerror due to a step in input frequency.Figure 8-17a [C ext > Ccrit- R ext = 0]CRITICALLY DAMPED ~ ~ 1Figure 8-17bOVERDAMPED ~ ~ 10MEASUREMENT SETUP FOR DISPLAYOF LOOP TRANSIENT RESPONSEFigure 8-17e [C < c crit' R ext > 0]HIGHLY OVERDAMPED ~ > 10Figure 8-16Figure 8-17d [C « c crit' R ext= 0)28

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