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By William F. Egan(auth.)
Broad-based and hands-on, Phase-Lock fundamentals, moment variation is either effortless to appreciate and simple to customise. The textual content can be utilized as a theoretical advent for graduate scholars or, while used with MATLAB simulation software program, the e-book turns into a digital laboratory for operating execs who are looking to increase their realizing of the layout technique and use it on the calls for of particular occasions. This moment version contains a huge physique of latest statistical facts got from simulations and makes use of to be had experimental information for affirmation of the simulation results.Content:
Chapter 1 creation (pages 1–13):
Chapter 2 the elemental Loop (pages 15–27):
Chapter three Loop parts (pages 29–57):
Chapter four Loop reaction (pages 59–69):
Chapter five Loop balance (pages 71–86):
Chapter 6 temporary reaction (pages 87–109):
Chapter 7 Modulation reaction (pages 111–136):
Chapter eight Acquisition (pages 137–169):
Chapter nine Acquisition Aids (pages 171–188):
Chapter 10 functions and Extensions (pages 189–229):
Chapter eleven section Modulation through Noise (pages 231–250):
Chapter 12 reaction to part Noise (pages 251–270):
Chapter thirteen illustration of Additive Noise (pages 271–286):
Chapter 14 Loop reaction to Additive Noise (pages 287–296):
Chapter 15 Phase?Locked Loop as a Demodulator (pages 297–317):
Chapter sixteen Parameter edition as a result of Noise (pages 319–333):
Chapter 17 Cycle Skipping as a result of Noise (pages 335–357):
Chapter 18 Nonlinear Operation in a Locked Loop (pages 359–376):
Chapter 19 Acquisition Aids within the Presence of Noise (pages 377–393):
Chapter 20 Bandlimited Noise (pages 395–413):
Chapter 21 additional details (pages 415–421):
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Additional resources for Phase-Lock Basics, Second Edition
Example text
JWDD062-02 JWDD062-Egan 24 August 16, 2007 17:31 Char Count= 0 2 THE BASIC LOOP Fig. 7 Mathematical block diagram of the simple loop with frequency variables as input and output. results as follows: ϕout (s) sϕout (s) ωout (s) = = . 27) A similar relationship holds for error responses. It is apparent from Figs. 28c) so that the output can easily be obtained from error and vice versa in most cases. 2. 5◦ ϕin 1 + j4899/1000 as before. 4 BODE PLOT One of the most important tools with which we will work is a logarithmic plot of openloop gain |G F G R | and phase shift G F G R versus modulation frequency, s → ωm .
3 Charge-Pump Phase Detector One widely used type of PD has a characteristic like the flip-flop PD, as shown in Fig. 1c, except for one very important addition [Gardner, 1980; Egan, 1981, pp. 115– 123; Egan, 2000, pp. 197–211]. It generates two different pulse outputs, one when the transition of v(B) lags that of v(A), as shown in Fig. 1b, and another when it JWDD062-03 JWDD062-Egan 32 August 16, 2007 15:17 Char Count= 0 3 LOOP COMPONENTS leads. ) The normal operating point is near-zero phase difference (τ = 0).
Sometimes an actual switched current source is used, as illustrated in Fig. 5a. Sometimes voltages are switched and converted to current by a resistor, as illustrated in Fig. 5b. In the first case the PD gain is K p = I /cycle, since the average current would be ±I if the phase error were ±1 cycle and would be 0 for 0 phase error, and the characteristic is linear between these points. Similarly, in the second case, if Vx = 0, the PD gain Fig. 3 Charge-pump waveforms. 1 PHASE DETECTOR 33 Fig. 4 Charge-pump phase detector characteristic.