Page 264 - Phase-Locked Loops Design, Simulation, and Applications
P. 264

MIXED-SIGNAL PLL APPLICATIONS PART 1: INTEGER-N FREQUENCY
             SYNTHESIZERS   Ronald E. Best                                                          156



























                      Figure 6.23 Output current versus time for a charge pump PFD.

             ourselves on calculating the fundamental only—in other words, the spur at an offset f  from
                                                                                                ref
             the carrier frequency f . First, we want to compute the fundamental of the current waveform in
                                  0
             Fig. 6.23. When we assume that the time intervals T  and T        are much shorter than the
                                                                 ov      comp
             reference period 1/f , the Fourier series yields the absolute value of the fundamental k
                                                                                                1
                               ref


                                                                                         (6.40)

               Next, we have to compute the fundamental of the AC signal at the output of the loop filter.
             Assuming that a first-order loop filter (Fig. 2.17b) is used, we have



                                                                                         (6.41)

             with  u f,ac,1  = fundamental of AC signal and  ω  = 2π f  and  F(f ) = transfer function
                                                                      ref
                                                                                 ref
                                                            ref
             (transfer impedance) of the loop filter. In most cases, the reference frequency is much higher
             than 1/τ  = 1/R C , thus F(f ) ≈ R . We can now compute the modulated radian frequency
                    2      2 1          ref     2
             ω (t) generated by the VCO
              2


                                                                                         (6.42)

               By integration over time we get the phase φ (t) of the VCO output signal
                                                         2


                                                                                         (6.43)
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