Resonant Frequency (LC) Calculator

Calculate LC tank circuit resonant frequency, quality factor, bandwidth, and characteristic impedance. Includes frequency sweep table and Q factor visualization.

Ω
Ω
Resonant Frequency (f₀)
1.5915 MHz
1,591,549.43 Hz
Angular Frequency (ω₀)
10,000,000.00 rad/s
ω₀ = 2πf₀
Quality Factor (Q)
10.000
Low Q — broad resonance
Bandwidth (BW)
159.1549 kHz
1.5120 MHz – 1.6711 MHz
Characteristic Impedance (Z₀)
1,000.0000 Ω
Z₀ = √(L/C)
Period
0.6283 μs
Wavelength: 188.50 m

Reactance at Resonance

Inductive Reactance (X_L)
1,000.0000 Ω
X_L = ωL
Capacitive Reactance (X_C)
1,000.0000 Ω
X_C = 1/(ωC)

Q Factor Visualization

Low Q (broad)High Q (sharp)
Q = 10.00

Frequency Sweep Reference

MultiplierFrequencyX_L (Ω)X_C (Ω)Net Reactance
0.25× f₀397.8874 kHz250.004,000.00-3,750.00
0.5× f₀795.7747 kHz500.002,000.00-1,500.00
0.75× f₀1.1937 MHz750.001,333.33-583.33
1× f₀1.5915 MHz1,000.001,000.00-0.00
1.25× f₀1.9894 MHz1,250.00800.00450.00
1.5× f₀2.3873 MHz1,500.00666.67833.33
2× f₀3.1831 MHz2,000.00500.001,500.00
Planning notes, formulas, and examples

About the Resonant Frequency (LC) Calculator

An LC circuit — also called a tank circuit or resonant circuit — consists of an inductor (L) and a capacitor (C) connected together. At a specific frequency, the inductive reactance and capacitive reactance cancel each other out, producing resonance. This resonant frequency is given by the formula f₀ = 1/(2π√(LC)).

LC circuits are the backbone of radio receivers, oscillators, filters, and frequency-selective networks. When tuned to resonance, these circuits can selectively amplify or reject signals at a particular frequency while ignoring all others. The sharpness of this frequency selection is characterized by the quality factor, Q.

This calculator determines the resonant frequency, angular frequency, Q factor, bandwidth, and characteristic impedance of an LC circuit. It also provides a frequency sweep reference table showing how inductive and capacitive reactance vary across a range of frequencies around resonance, and a visual representation of the Q factor to help you understand the selectivity of your circuit.

When This Page Helps

Designing radio filters, oscillators, or matching networks requires precise knowledge of the resonant frequency and Q factor. Manual calculations with unit conversions between henries, microhenries, farads, and picofarads are tedious and error-prone. This calculator handles all unit conversions automatically and provides a comprehensive analysis including bandwidth, impedance matching data, and a frequency sweep table — everything you need for LC circuit design in one place.

How to Use the Inputs

  1. Enter the inductance value and select the appropriate unit (H, mH, μH, or nH).
  2. Enter the capacitance value and select the appropriate unit (F, mF, μF, nF, or pF).
  3. Optionally enter source and load resistance values for Q factor and bandwidth calculations.
  4. Click a preset button to load common LC configurations (AM radio, FM radio, WiFi, etc.).
  5. Read the resonant frequency, Q factor, bandwidth, and characteristic impedance from the output cards.
  6. Review the frequency sweep reference table to see reactance behavior across the frequency range.
  7. Use the Q factor bar to quickly assess if the circuit is narrowband or wideband.
Formula used
Resonant Frequency: f₀ = 1 / (2π√(LC)) ω₀ = 2πf₀ = 1/√(LC) Quality Factor: Q = Z₀ / R_total = (1/R)√(L/C) Bandwidth: BW = f₀ / Q Characteristic Impedance: Z₀ = √(L/C) Reactances at frequency f: X_L = 2πfL X_C = 1/(2πfC)

Example Calculation

Result: 1.592 MHz

With L = 100 μH and C = 100 pF, the resonant frequency is f₀ = 1/(2π√(100×10⁻⁶ × 100×10⁻¹²)) ≈ 1.592 MHz. At this frequency, inductive and capacitive reactances are equal at about 1000 Ω, so the characteristic impedance Z₀ ≈ 1000 Ω.

Tips & Best Practices

  • Use high-Q inductors (low DC resistance) for sharper selectivity in filter applications.
  • Parasitic capacitance in inductors and lead inductance in capacitors shift the actual resonance — measure with a network analyzer for precision work.
  • For a parallel LC circuit, impedance is maximum at resonance; for series LC, impedance is minimum.
  • Temperature changes affect both L and C values, which can drift the resonant frequency — use NP0/C0G capacitors for stability.
  • The 3 dB bandwidth of the resonant peak is f₀/Q, so higher Q means narrower bandwidth.
  • When designing bandpass filters, cascade multiple LC stages to achieve steeper roll-off.

LC Circuit Applications in Modern Electronics

LC circuits remain essential building blocks despite the dominance of digital electronics. In RF (radio frequency) design, ceramic and SAW filters have replaced discrete LC filters for many applications, but understanding LC resonance is still fundamental to designing matching networks, voltage-controlled oscillators (VCOs), and antenna tuning circuits. In power electronics, LC filters smooth rectified AC into clean DC, and resonant converters use LC tanks to achieve zero-voltage switching for high efficiency.

Series vs. Parallel LC Circuits

A series LC circuit presents minimum impedance at resonance — it acts as a short circuit for signals at f₀ while blocking other frequencies. This makes it ideal for notch (band-reject) filters in the signal path. A parallel LC circuit presents maximum impedance at resonance, making it suitable for bandpass filters when placed in shunt configuration. The distinction is crucial for filter topology selection.

Practical Considerations for LC Design

Real inductors have parasitic resistance (DCR) and self-capacitance, while real capacitors have equivalent series resistance (ESR) and inductance (ESL). These parasitics create a self-resonant frequency above which components behave oppositely — inductors become capacitive and capacitors become inductive. Always check that your operating frequency is well below the component self-resonant frequency. At microwave frequencies, transmission line sections often replace discrete LC elements.

Sources & Methodology

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Frequently Asked Questions

  • An LC tank circuit consists of an inductor and capacitor connected in parallel (or series). Energy oscillates between the magnetic field of the inductor and the electric field of the capacitor at the resonant frequency. It is called a "tank" because it stores energy like a tank stores fluid.