Step 1: The poles of the system are given by the eigenvalues of the matrix \( A \).
Step 2: The characteristic equation is found by solving: \[ \det(A - \lambda I) = 0 \]
Step 3: Substituting \( A = \begin{bmatrix} 0 & 3 \\ 3 & 0 \end{bmatrix} \): \[ \begin{vmatrix} 0 - \lambda & 3 \\ 3 & 0 - \lambda \end{vmatrix} = 0 \]
Step 4: Computing the determinant: \[ (-\lambda)(-\lambda) - (3 \times 3) = \lambda^2 - 9 = 0 \]
Step 5: Solving for \( \lambda \): \[ \lambda^2 = 9 \] \[ \lambda = \pm j3 \]
Step 6: The poles of the system are at \( s = \pm j3 \).
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: