The standard second-order form is:
\[
G(s) = \frac{\omega_n^2}{s^2 + 2\zeta\omega_n s + \omega_n^2}.
\]
System 1:
\[
s^2 + s + 1 \Rightarrow 2\zeta\omega_n = 1,\ \omega_n^2 = 1.
\]
Thus:
\[
\omega_n = 1,\quad \zeta = \frac{1}{2}.
\]
System 2:
\[
s^2 + s\sqrt{10} + 10 \Rightarrow 2\zeta\omega_n = \sqrt{10},\ \omega_n^2 = 10.
\]
Thus:
\[
\omega_n = \sqrt{10}, \quad
\zeta = \frac{\sqrt{10}}{2\sqrt{10}} = \frac{1}{2}.
\]
Both systems have the same damping ratio $\zeta = 0.5$.
Percentage overshoot depends ONLY on \(\zeta\), so both systems have identical overshoot.
→ (A) is true.
Steady-state value with unit step:
\[
\lim_{s\to 0} sG(s)\frac{1}{s} = G(0) = \frac{10}{1} = 10 \quad \text{and} \quad G_2(0)=1.
\]
Different.
→ (B) false.
Damped frequency:
\[
\omega_d = \omega_n\sqrt{1-\zeta^2}.
\]
Since \(\omega_n\) differs, they are not equal → (C) false.
Settling time:
\[
T_s \approx \frac{4}{\zeta\omega_n}.
\]
Different \(\omega_n\) → different \(T_s\).
→ (D) false.
Final Answer: (A)