6122 CHAPTER 6. THE FREQUENCY-RESPONSE DESIGN METHOD
Problems and Solutions for Section 6.7
44. For the lead compensator
Dc(s) = TDs+ 1
TDs+ 1;
where < 1.
(a) Show that the phase of the lead compensator is given by
= tan1(TD!)tan1(TD!):
(b) Show that the frequency where the phase is maximum is given by
!max =1
TDp;
and that the maximum phase corresponds to
sin max =1
1 + :
(c) Rewrite your expression for !max to show that the maximum-phase
frequency occurs at the geometric mean of the two corner frequencies
on a logarithmic scale:
log !max =1
2log 1
TD
+ log 1
TD:
(d) To derive the same results in terms of the pole-zero locations, rewrite
Dc(s)as
Dc(s) = s+z
s+p;
and then show that the phase is given by
= tan1!
jzjtan1!
jpj;
such that
!max =pjzjjpj:
Hence the frequency at which the phase is maximum is the square
root of the product of the pole and zero locations.