RLC Resonance — Series, Parallel & Harmonics
At resonance, inductive and capacitive reactances cancel and the circuit's behavior flips: a series RLC becomes a short (current spikes, L and C voltages magnify), while a parallel RLC becomes an open (impedance peaks, branch currents circulate). Sweep the components, find the resonant frequency, and see why a capacitor bank that resonates on a harmonic is a power-system hazard.
Both topologies resonate when the reactances are equal and opposite, ωL = 1/ωC:
Series RLC (voltage source). At f₀ the reactances cancel, leaving only R, so impedance is minimum and current is maximum. The catch: the L and C voltages don't cancel internally — each rises to Q × source voltage. High Q means dangerous voltage magnification across the capacitor.
Parallel RLC (current source). At f₀ the branch susceptances cancel, so impedance is maximum (= R). A small source current produces a large node voltage, and the L and C branches carry a circulating current of Q × source current — even though the line current is small. Note Q rises with R here (light damping = sharp, dangerous peak), the opposite of the series case.