The solid curves in Figure 7–96 show the magnitude curve and phase-angle curve for the compen-
sated system. Note that the bandwidth is approximately equal to the gain crossover frequency. The
lead compensator causes the gain crossover frequency to increase from 6.3 to 9 radsec. The in-
crease in this frequency means an increase in bandwidth. This implies an increase in the speed of
response. The phase and gain margins are seen to be approximately 50° and ±qdB, respectively.
The compensated system shown in Figure 7–97 therefore meets both the steady-state and the
relative-stability requirements.
Note that for type 1 systems, such as the system just considered, the value of the static veloc-
ity error constant Kvis merely the value of the frequency corresponding to the intersection of
the extension of the initial –20-dBdecade slope line and the 0-dB line, as shown in Figure 7–96.
Note also that we have changed the slope of the magnitude curve near the gain crossover frequency
from–40dBdecade to –20dBdecade.Section 7–11 / Lead Compensation 49940200- 20
- 40
0 °- 90 °
- 180 °
Gc
10
Kv50 °1246v in rad/sec10 20 40 60 100Gc
10GcGGcG- 6 dB
G 1 = 10 GG 1 = 10 GdBFigure 7–96
Bode diagram for the
compensated system.
4
s(s+ 2)41.7(s+ 4.41)
s+ 18.4+- Figure 7–97
Compensated
system.