Step 1: The number of root locus asymptotes is given by: \[ N_a = P - Z \] where \( P \) is the number of poles and \( Z \) is the number of zeros.
Step 2: Given: - \( P = 4 \) (number of poles) - \( Z = 2 \) (number of zeros) \[ N_a = 4 - 2 = 2 \]
Step 3: The angles of asymptotes are determined using the formula: \[ \theta_k = \frac{(2k + 1) 180^\circ}{N_a}, \quad k = 0, 1, \dots, (N_a - 1) \]
Step 4: Substituting \( N_a = 2 \): \[ \theta_0 = \frac{(2 \times 0 + 1) 180^\circ}{2} = 90^\circ \] \[ \theta_1 = \frac{(2 \times 1 + 1) 180^\circ}{2} = -90^\circ \]
Step 5: Thus, the two asymptotes move towards infinity along \( \pm 90^\circ \).
The motion of electrons in a CRT is due to:
The direction of current flow in the circuit is such that the induced magnetic field produced by the induced current will oppose the original magnetic field. This is:
The electromagnetic wave propagates in free space with a speed of:
A closed-loop system has the characteristic equation given by: $ s^3 + k s^2 + (k+2) s + 3 = 0 $.
For the system to be stable, the value of $ k $ is: