Series RLC circuit step response under square wave excitation | Adjust \(R, L, C\) to observe underdamped (oscillatory decay), critically damped, and overdamped states
Underdamped (\(\zeta < 1\)): \(v_C(t)\) oscillates with decay, overshoot increases as \(\zeta\) decreases. Poles are a pair of complex conjugates.
Critically Damped (\(\zeta = 1\)): Fastest non-overshooting response, \(v_C(t)\) rises monotonically without oscillation. Poles are repeated real roots.
Overdamped (\(\zeta > 1\)): Response rises slowly and monotonically, no oscillation. Poles are two distinct negative real roots.
\(\zeta = \frac{R}{2}\sqrt{\frac{C}{L}}\), \(\omega_0 = \frac{1}{\sqrt{LC}}\)
\(\omega_d = \omega_0\sqrt{1-\zeta^2}\) (underdamped)
Overshoot \(M_p = e^{-\pi\zeta/\sqrt{1-\zeta^2}} \times 100\%\)
Poles: \(s_{1,2} = -\zeta\omega_0 \pm \omega_0\sqrt{\zeta^2-1}\)