Page 66 - Phase-Locked Loops Design, Simulation, and Applications
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MIXED-SIGNAL PLL ANALYSIS   Ronald E. Best                                              47

               we get the normalized form



                                                                                           (3.24)



               This is identical to the phase-transfer function we obtained for the PLL using a phase detector
               with voltage output [cf. Eq. (3.18)].



               Transient Response of the PLL in the Locked State


               Knowing the phase-transfer function H(s) and the error-transfer function H (s) of the PLL, we
                                                                                        e
               can calculate its response on the most important excitation signals. We therefore analyze the
               PLLs answer to

               ■ A phase step
               ■ A frequency step
               ■ A frequency ramp

               applied to its reference input.


               Phase step applied to the reference input
               A reference signal performing a phase step at time t = 0 has been shown in Fig. 2.2a. In this
               case, the phase signal θ (t) is a step function,
                                     1


                                                                                           (3.25)


               where  u(t) is the unit step function and  ΔΦ is the size of the phase step. For the Laplace
               transform Θ (s), we therefore get
                           1



                                                                                           (3.26)

                 The phase error θ  is obtained from
                                  e


                                                                                           (3.27)

                 Inserting Eq. (3.20) into Eq. (3.27) yields



                                                                                           (3.28)



                 Applying the inverse Laplace transform to Eq. (3.28), we get the phase error functions θ (t)
                                                                                                       e
               shown in Fig. 3.5. The phase error has been normalized to the phase step ΔΦ.
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