Phase Lead Compensator
A phase lead compensator adds positive phase shift to the open-loop frequency response over a certain frequency range. Its typical transfer function is:
\[ G_c(s) = K_c \frac{s+z}{s+p} \quad \text{where } p > z \]
Alternatively, a normalized form is often used:
\[ G_c(s) = \alpha \frac{1 + sT}{1 + s\alpha T} \quad \text{with } \alpha < 1 \]
This means:
- Zero at \( s = -1/T \)
- Pole at \( s = -1/(\alpha T) \)
- Since \( \alpha < 1 \), \( 1/(\alpha T) > 1/T \) ⇒ pole is further left
Effects of a Phase Lead Compensator
- (a) Bandwidth increases: ✅ True. The gain crossover frequency increases, expanding the bandwidth.
- (b) High frequency gain decreases: ❌ False. The gain at high frequencies tends to be equal to or higher than the DC gain. For example: \[ G_c(s) = \alpha \frac{1 + sT}{1 + s\alpha T} \Rightarrow \lim_{s \to \infty} G_c(s) = 1 \] \[ \lim_{s \to 0} G_c(s) = \alpha < 1 \Rightarrow \text{High-frequency gain > DC gain} \] Hence, the gain at high frequencies increases or stays constant compared to DC. This statement is incorrect.
- (c) Dynamic response becomes faster: ✅ True. Greater bandwidth generally implies improved transient characteristics, such as reduced rise and settling times.
- (d) Susceptible to high frequency noise: ✅ True. The boost in gain at higher frequencies can amplify noise, making the system more sensitive to high-frequency disturbances.
Conclusion
\[ \boxed{\text{Incorrect statement: (b) High frequency gain decreases}} \]