Parallel (Tank) Resonant Frequency

f = (1/2π)·√(1/LC − R²/L²)

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Result

Formula

f = (1/2π) × √(1/(LC) − R²/L²)

Description

A real parallel LC "tank" circuit resonates slightly below the ideal 1/(2π√LC) because the coil’s series resistance shifts the resonant frequency. At resonance the tank impedance is maximum (anti-resonance), which is why parallel resonant circuits are used as frequency-selective loads in oscillators, RF amplifiers, and traps. When R is small the correction term is negligible.

Variables

  • f — Parallel resonant frequency (Hz)
  • L — Inductance (H)
  • C — Capacitance (F)
  • R — Series resistance of the coil (Ω)

Practical Notes

For a high-Q coil (small R) this reduces to the familiar f = 1/(2π√LC). The term R²/L² must stay below 1/LC or the circuit is overdamped and does not resonate.