The formula
f₀ = 1 / (2π√(LC)) ; Z₀ = √(L/C) ; Q = Z₀/R ; BW = f₀/Q
- f₀
- resonant frequency (hertz)
- L
- inductance (henries)
- C
- capacitance (farads)
- Q
- quality factor — sharpness of the resonance (dimensionless)
- BW
- −3 dB bandwidth around f₀ (hertz)
Worked example
L = 100 mH, C = 10 µF, with 10 Ω of series resistance.
- LC = 0.1 × 10 × 10⁻⁶ = 1 × 10⁻⁶, so √(LC) = 1 × 10⁻³
- f₀ = 1 / (2π × 10⁻³) = 159.2 Hz
- Z₀ = √(0.1 / 10⁻⁵) = √10000 = 100 Ω
- Q = 100 / 10 = 10, so BW = 159.2 / 10 = 15.9 Hz
f₀ = 159.2 Hz with Q = 10 and a 15.9 Hz bandwidth.
Where you'll use it
Radio tuning, filter and oscillator design, and the exam favourite about current at resonance in a series RLC circuit. Lower series resistance means higher Q and a sharper, narrower peak.