Calculate LC tank circuit resonant frequency, quality factor, bandwidth, and characteristic impedance. Includes frequency sweep table and Q factor visualization.
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.
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.
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)
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.
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.
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.
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.
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.
The Q factor is determined by the ratio of energy stored to energy dissipated per cycle. In practical terms, Q = Z₀/R where Z₀ = √(L/C) and R is the total resistance in the circuit. Higher Q means less energy loss and sharper resonance.
Yes, both series and parallel LC circuits resonate at the same frequency f₀ = 1/(2π√(LC)). However, their behavior at resonance differs: a series LC circuit has minimum impedance at resonance, while a parallel LC circuit has maximum impedance.
Radio receivers use variable capacitors or inductors to change the LC resonant frequency, selecting different broadcast stations. Each station transmits at a specific frequency, and the LC circuit acts as a bandpass filter to isolate that signal from all others.
Interestingly, swapping the inductance and capacitance values produces the same resonant frequency because the formula uses the product L×C. However, the characteristic impedance Z₀ = √(L/C) and Q factor will be different.
Crystal oscillators behave like very high-Q LC circuits. While you can use this calculator to estimate the resonant frequency of the equivalent LC model, quartz crystals have Q factors of 10,000 to 1,000,000, far exceeding typical LC circuits.