
Concept:& nbsp;
For a standard second-order system, \[ s^2+2\zeta\omega_n s+\omega_n^2=0, \] the location of poles in the \(s\)-plane determines the nature of damping. The damping ratio \(\zeta\) classifies the system as underdamped, critically damped, overdamped, or undamped.& nbsp;
Step 1: Recall the pole locations.
The roots of the characteristic equation are \[ s=-\zeta\omega_n \pm j\omega_n\sqrt{1-\zeta^2}. \] The nature of the system depends on \(\zeta\): \[ \begin{array}{|c|c|} \hline \zeta & \text{Nature of System} \\ \hline 0 & \text{Undamped} \\ 0<\zeta<1 & \text{Underdamped} \\ 1 & \text{Critically Damped} \\ \zeta>1 & \text{Overdamped} \\ \hline \end{array} \]& nbsp;
Step 2: Interpret the given pole location.
The figure shows a circle of radius \[ \omega_n \] centered at the origin of the \(s\)-plane. The marked poles lie on the imaginary axis at \[ s=\pm j\omega_n. \] Hence, \[ \operatorname{Re}(s)=0. \] Comparing with \[ s=-\zeta\omega_n \pm j\omega_n\sqrt{1-\zeta^2}, \] we obtain \[ -\zeta\omega_n=0. \] Since \(\omega_n \neq 0\), \[ \boxed{\zeta=0}. \]& nbsp;
Step 3: Determine the system type.
For \[ \zeta=0, \] the poles become \[ s=\pm j\omega_n. \] These poles are purely imaginary and produce sustained oscillations of constant amplitude. There is no exponential decay term, which means no damping is present. Therefore, the system is \[ \boxed{\text{Undamped}}. \]& nbsp;
Step 4: Verify using the time response.
For an undamped system, \[ c(t)=A\sin(\omega_n t)+B\cos(\omega_n t). \] The oscillations continue indefinitely without reduction in amplitude, confirming that \[ \boxed{\zeta=0}. \]& nbsp;
Final Answer: \[ \boxed{\zeta=0} \] and therefore \[ \boxed{\text{Undamped System}} \] Hence, the correct option is \[ \boxed{\text{(D)}} \]
| \( S^n \) | Col 1 | Col 2 | Col 3 |
|---|---|---|---|
| \( S^5 \) | 2 | 1 | |
| \( S^4 \) | 3 | 2 | 1 |
| \( S^3 \) | \(-\frac{4}{3}\) | \(-\frac{2}{3}\) | |
| \( S^2 \) | \(\frac{1}{2}\) | 1 | |
| \( S^1 \) | 2 | ||
| \( S^0 \) | 1 |