Step 1: A phase lag compensator is used to improve the steady-state accuracy of a control system while reducing bandwidth and increasing stability margins.
Step 2: The general form of a phase lag compensator is: \[ G_c(s) = K \frac{(s + a)}{(s + b)} \] where: - \( a \) represents the zero of the compensator. - \( b \) represents the pole of the compensator.
Step 3: Phase lag compensators are characterized by:
- A pole (\( b \)) closer to the origin than the zero (\( a \)).
- This ensures that at lower frequencies, the compensator reduces the phase angle, introducing a negative phase shift.
Step 4: The condition for a phase lag compensator is: \[ a<b \] which ensures that the pole is dominant and the system experiences phase lag.
A proton is moving undeflected in a region of crossed electric and magnetic fields at a constant speed of \( 2 \times 10^5 \, \text{m/s} \). When the electric field is switched off, the proton moves along a circular path of radius 2 cm. The magnitude of electric field is \( x \times 10^4 \, \text{N/C} \). The value of \( x \) is \(\_\_\_\_\_\). (Take the mass of the proton as \( 1.6 \times 10^{-27} \, \text{kg} \)).
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: