Resonance Frequency Calculator

Resonance occurs when a system oscillates at maximum amplitude at a specific frequency — the resonant (or natural) frequency. In LC circuits, energy alternates between the inductor's magnetic field and the capacitor's electric field: f = 1/(2π√(LC)). Adding resistance forms an RLC circuit with finite bandwidth and a quality factor Q = (1/R)√(L/C) for series circuits. For mechanical systems, a mass on a spring oscillates at its natural frequency f_n = (1/2π)√(k/m), where k is the spring constant and m is the mass. Understanding resonance is critical in electronics (tuned filters, oscillators, radio receivers), mechanical engineering (vibration isolation, structural analysis), and acoustics (musical instruments, speaker design). This calculator covers all three scenarios with selectable units and full formula display.

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LC Circuit Inputs

Results

Enter L and C to calculate resonant frequency

lightbulb Tips

  • f = 1/(2π√(LC)) for LC circuits
  • Q = (1/R)√(L/C) — higher Q = narrower bandwidth
  • f_n = (1/2π)√(k/m) for spring-mass systems
  • Halve L or C → frequency rises by √2 ≈ 1.414×

How to Use This Calculator

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Choose Calculator Mode

Select LC Circuit for a simple inductor-capacitor tank circuit, RLC Circuit to also get Q factor and bandwidth with a resistor, or Mechanical for a spring-mass natural frequency.

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Enter Component Values

Type the inductance (H/mH/µH/nH), capacitance (F/mF/µF/nF/pF), or spring constant and mass. All common unit prefixes are supported.

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Read Resonant Frequency

The resonant frequency is displayed in Hz, kHz, MHz, or GHz automatically scaled to the most readable unit. The period (1/f) is also shown.

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Check Q Factor & Bandwidth (RLC)

For RLC mode, the Q factor and bandwidth tell you how selective your circuit is. High Q = narrow bandwidth = more selective filter.

The Formula

In an LC circuit, energy oscillates between the inductor (magnetic) and capacitor (electric) at f = 1/(2π√(LC)). Adding resistance (RLC) damps the oscillation — the Q factor Q = (1/R)√(L/C) describes how sharp the resonance peak is. High Q means narrow bandwidth and low energy loss. For a spring-mass system, the analogous formula is f_n = (1/2π)√(k/m), where k is the spring stiffness and m is the suspended mass. Both formulas share the same mathematical structure.

f = 1/(2π√(LC)) | f_n = (1/2π)√(k/m) | Q = (1/R)√(L/C)

lightbulb Variables Explained

  • f Resonant frequency (Hz)
  • L Inductance (H — henries)
  • C Capacitance (F — farads)
  • R Resistance (Ω — ohms) for RLC circuits
  • k Spring constant (N/m) for mechanical systems
  • m Mass (kg) for mechanical spring-mass system
  • Q Quality factor — sharpness of resonance peak (dimensionless)
  • BW Bandwidth (Hz) — frequency range around resonance: BW = f/Q

tips_and_updates Pro Tips

1

Halving L or C raises frequency by √2 (≈1.414×). To double frequency, reduce L or C to ¼ of original value.

2

High Q (>10) means a sharp, selective resonance — ideal for radio filters. Low Q (<1) means broad, overdamped response.

3

For spring-mass: doubling the mass lowers natural frequency by √2. Doubling spring stiffness raises it by √2.

4

A Q factor of 1/(2ζ) relates to the damping ratio ζ — critical damping is ζ=1 (Q=0.5), underdamped is ζ<1 (Q>0.5).

5

Real LC circuits always have some resistance (wire/coil ESR) — the Q factor drops and bandwidth widens with higher R.

Frequently Asked Questions

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Data sourced from trusted institutions

All formulas verified against official standards.