Compute the natural resonance of any LC tank circuit. Enter inductance, capacitance, and optional series resistance to obtain f₀, ω₀, Q factor, and visualize the normalized amplitude response curve.
An LC circuit (also called a tank circuit or tuned circuit) consists of an inductor (L) and a capacitor (C) connected together. When energy oscillates between the magnetic field of the inductor and the electric field of the capacitor, the circuit exhibits resonance at a specific natural frequency. This frequency is the cornerstone of radio tuners, oscillators, filters, and impedance matching networks.
$$ f₀ = \frac{1}{2\pi\sqrt{LC}} \quad \text{Hz} $$
Angular frequency: ω₀ = 2πf₀ = 1/√(LC) rad/s
The formula is derived from setting inductive reactance (XL = ωL) equal to capacitive reactance (XC = 1/(ωC)). At resonance, the net reactance cancels, and impedance becomes purely resistive (equal to the parasitic resistance R). This phenomenon maximizes current in a series RLC circuit and maximizes voltage in a parallel RLC configuration.
The quality factor Q quantifies the sharpness of resonance: Q = ω₀L / R (series) or Q = R / (ω₀L) (parallel). Higher Q means narrower bandwidth and greater frequency selectivity. For an ideal lossless circuit (R=0), Q → ∞ and oscillations sustain indefinitely — a theoretical boundary. Our calculator computes Q based on your input resistance (real-world component ESR or external resistor).
| Application | Inductance | Capacitance | Resonant Frequency |
|---|---|---|---|
| AM broadcast (520–1610 kHz) | 240 µH | 100–365 pF | ~540 kHz – 1 MHz |
| FM broadcast (88–108 MHz) | 100 nH | 10–20 pF | ~89–112 MHz |
| 2.4 GHz WLAN/BT | 2.2 nH | 2.2 pF | ~2.41 GHz |
| Audio crossover notch filter | 10 mH | 0.1 µF | ~5.03 kHz |
| Low-frequency power oscillator | 500 µH | 1 µF | ~7.12 kHz |
Sir William Thomson (Lord Kelvin) and later Oliver Heaviside formalized the resonance equation in the 19th century. The expression ω = 1/√(LC) emerges from solving the second-order differential equation for an LC loop: L(d²i/dt²) + (1/C)i = 0. The sinusoidal solution reveals the natural frequency. Modern RF design relies on this relationship to stabilize oscillators and ensure minimal phase noise. The Euler line analogy does not apply, but the elegance of LC resonance permeates nearly every wireless device.