LC Resonant Frequency Calculator
Calculate the resonant frequency of an LC tank circuit (f = 1/(2π√LC)), plus Q factor and bandwidth for a damped RLC network.
How to Use
- Enter inductance L and capacitance C.
- Optionally enter resistance R for damped RLC Q-factor.
- Resonant frequency f₀ = 1/(2π√(LC)) appears with impedance at resonance.
Show Work
Formulas
History of LC Resonance
William Thomson (later Lord Kelvin) derived the formula f = 1 / (2π√LC) in 1853 while analyzing the oscillations of charge in a Leyden jar discharged through a coil — one of the earliest studied examples of a physical oscillator. Thomson's formula predicted the ringing discharge Joseph Henry had observed two decades earlier and is still often called "Thomson's formula" in European texts.
The practical impact came half a century later. When Heinrich Hertz generated and detected radio waves in 1888, both transmitter and receiver relied on resonant LC tanks. Guglielmo Marconi's early spark-gap radios (1895 onward) were shotgun-wide in bandwidth until resonant tuning was added around 1900 — allowing multiple stations to share the airwaves by transmitting and receiving on different LC resonant frequencies. Every radio receiver since has been a cascade of tuned resonant networks, and the same formula governs crystal oscillators, wireless charging pads, quartz watch timing elements, and MRI gradient coils.
Q-factor as a quantitative figure of merit was introduced by K. S. Johnson at Bell Labs in 1914 — he chose the letter Q arbitrarily (no, it does not stand for "quality"). High Q means a narrow, selective resonance; low Q means a broad, well-damped one. Air-core coils and vacuum capacitors push Q to the thousands; crystals and surface-acoustic-wave resonators reach tens of thousands; superconducting cavities in particle accelerators hit 1010.
About This Calculator
Enter inductance L and capacitance C with engineering suffixes (nH, µH, mH, pF, nF, µF). The calculator returns the resonant frequency via Thomson's formula, the characteristic impedance Z0 = √(L/C), and — if you supply a series resistance R — the quality factor Q and −3 dB bandwidth BW = f0/Q.
Real resonators deviate from the ideal: wire DC resistance in the inductor, ESR in the capacitor, core loss, and radiation from open coils all add damping. Q below 10 is common for PCB inductors; Q of 100+ requires air-core or carefully chosen RF parts; Q above 1000 needs crystals or acoustic resonators. Everything runs client-side; no values leave your browser.
Frequently Asked Questions
What is resonance?
The frequency at which Xl = Xc for an LC circuit. Current and voltage are in phase; impedance is minimum (series) or maximum (parallel). Used in oscillators, filters, and antennas.
Why care about Q?
Q = f₀/BW. High Q = narrow resonance peak = selective filter. Low Q = broad response. Set by R (lower R = higher Q in series RLC).
What about parasitic resistance?
All real inductors have DC resistance; capacitors have ESR. These damp the resonance, limiting practical Q to a few hundred without special (air-core, vacuum cap) components.
Common Use Cases
Radio Receiver
Tuned RF front-end with adjustable C to select station frequency.
Wireless Charging
Transmit and receive coils tuned to the same LC resonance for efficient coupling.
Crystal Oscillator Model
Crystal is a mechanical resonator modeled as series RLC with huge Q (10,000+).
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