Comparison

Series vs Parallel Resonance

A radio receiver's tuning circuit must reject a 98.3 MHz station while locking onto 98.7 MHz — that selectivity comes from resonance. Series resonance creates minimum impedance at the resonant frequency, making it useful for passing a band of signals. Parallel resonance creates maximum impedance, making it ideal for blocking or filtering. Both share the same resonant frequency formula but behave like electrical opposites under load.

EEE, ECE, EI

Side-by-side comparison

ParameterSeriesParallel Resonance
Resonant Frequencyf0 = 1 / (2π√LC) — same formulaf0 = 1 / (2π√LC) — same formula
Impedance at f0Minimum — purely resistive (Z = R)Maximum — purely resistive (Z = L/CR, called dynamic resistance)
Current at f0Maximum (I = V/R)Minimum (circulating current is Q times supply current)
Q-FactorQ = (1/R)√(L/C) = ω0L/RQ = R√(C/L) = R/ω0L (R is tank resistance)
BandwidthBW = f0/Q = R/(2πL)BW = f0/Q = 1/(2πRC)
Voltage MagnificationVoltage across L or C = Q × V_source (can be dangerous)Not applicable — current magnification instead
Current MagnificationNot applicableCirculating tank current = Q × I_supply
ApplicationSeries RLC filters, IF transformers at 455 kHzTank circuits in LC oscillators, RF amplifier loads at MHz range

Key differences

At resonance, both circuits present purely resistive impedance, but the values are opposite extremes. Series resonance gives Z_min = R (often a few ohms); parallel resonance gives Z_max = L/CR (can be hundreds of kilohms). Voltage magnification of Q times occurs across the inductor or capacitor in a series circuit — at 455 kHz IF with Q = 50, a 100 mV input produces 5 V across the capacitor. Parallel resonance magnifies circulating tank current by Q, not voltage. Q and bandwidth are inversely related in both cases.

When to use Series

Use series resonance when you need to pass or amplify a specific frequency with maximum current — for example, in the 455 kHz intermediate frequency transformer stage of an AM superheterodyne radio receiver.

When to use Parallel Resonance

Use parallel resonance when you need high impedance at a specific frequency to act as a high-Q bandpass filter or oscillator tank — for example, in a Colpitts oscillator at 10 MHz where the LC tank defines oscillation frequency.

Recommendation

For exam problems, always use f0 = 1/(2π√LC) for both circuits — that formula is the same. Then choose: series for minimum impedance and maximum current at f0; parallel for maximum impedance and minimum current at f0. That single distinction resolves nearly every MCQ on resonance.

Exam tip: Examiners always ask for dynamic resistance of a parallel circuit — remember Z_dynamic = L/(CR), not infinity, because real inductors have series resistance R.

Interview tip: Interviewers at analog design companies like Texas Instruments or Analog Devices ask about Q factor and bandwidth in the same breath — state that Q = f0 / BW and that a higher Q means sharper selectivity but narrower bandwidth.

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