100.0006
Hz
0.100001
kHz
628.3222
rad/s
0.01
s
6.2832
Ω
100.0006
Hz
0.100001
kHz
628.3222
rad/s
0.01
s
6.2832
Ω
The resonant frequency of an LC circuit is the frequency at which inductive and capacitive reactances are equal and opposite, causing them to cancel. At this frequency, the circuit oscillates most freely — with minimum impedance in series configuration and maximum impedance in parallel configuration. The resonant frequency formula is: f₀ = 1 / (2π√(LC)), where L is inductance in henries and C is capacitance in farads.
This fundamental formula is one of the most important in electrical engineering, governing the operating frequency of radio transmitters and receivers, oscillators, filters, resonant power converters, wireless charging systems, musical instrument pickups, and seismometers. The formula reveals that resonant frequency is inversely proportional to the square root of both inductance and capacitance — decreasing either L or C increases f₀, and vice versa.
The physical picture: energy oscillates between the inductor's magnetic field and the capacitor's electric field. When the capacitor is fully charged, all energy is electric (½CV²). The capacitor then discharges through the inductor, transferring energy to the magnetic field. When fully discharged, all energy is magnetic (½LI²). The inductor's collapsing field recharges the capacitor with opposite polarity, and the cycle repeats. Without resistance, this would continue indefinitely — with resistance, oscillations damp out exponentially at rate α = R/(2L).
The angular resonant frequency ω₀ = 2πf₀ = 1/√(LC) in radians per second is often more convenient for mathematical analysis involving Laplace transforms and phasor diagrams. Many circuit equations are simpler expressed in terms of ω than f.
The characteristic impedance Z₀ = √(L/C) in ohms is a property of the LC network that determines the voltage-to-current ratio of oscillations and the impedance transformation properties of the resonant circuit. In LC transmission line models, Z₀ equals the characteristic impedance of the equivalent transmission line. For LC matching networks, Z₀ determines the transformation ratio between source and load impedances.
Practical applications: AM radio tuning (f₀ varies from 535 kHz to 1,605 kHz by varying C with a variable tuning capacitor); LC oscillator circuits in clocks and communication systems; medical imaging (MRI resonant frequency f₀ = γB₀/2π depends on static magnetic field B₀ and gyromagnetic ratio γ); and inductive power transfer (Qi charging operates at 87–205 kHz, resonant at f₀ of the coil+capacitor tank).
f₀ = 1/(2π√(LC)) with L in henries (mH/1000) and C in farads (µF/1,000,000). Angular frequency ω₀ = 2πf₀. Period T = 1/f₀. Characteristic impedance Z₀ = √(L/C). Results given in Hz, kHz, rad/s, seconds, and ohms.
Higher L or C → lower f₀ (more energy storage per unit, slower oscillation). Lower L or C → higher f₀ (faster oscillation). Characteristic impedance Z₀ sets the 'natural' V/I ratio in the resonant circuit. Q factor = Z₀/R (for series circuit) — high Z₀ relative to R means high Q and sharp resonance. To shift f₀ up: reduce L or C. To shift f₀ down: increase L or C.
Inputs
Results
25 nH (0.025 mH) and 4.04 pF (4.04e-6 µF) resonates at exactly 100 MHz — the middle of the FM broadcast band (87.5–108 MHz). Characteristic impedance Z₀ = 2.5 Ω.
Inputs
Results
A 10 mH coil with 158.1 µF resonates at 127.3 kHz — within the Qi wireless charging operating range. Z₀ ≈ 8 Ω; with R = 1 Ω, Q ≈ 8.
Natural frequency ω_n = 1/√(LC) (rad/s) is the undamped frequency of the LC circuit with zero resistance. Resonant (damped) frequency ω_d = √(ω_n² - α²) is slightly lower due to damping. For high-Q circuits (low R), ω_d ≈ ω_n. The resonant frequency f₀ = ω_n/(2π) calculated here is the undamped natural frequency.
Adjust L or C (or both). Variable capacitors (air-variable or varactor diodes for electronic tuning) are most common. Start with a target frequency, select a practical L value, then calculate C = 1/(L × (2πf₀)²). Fine-tune with a small trimmer capacitor in parallel with the main C. For inductors, a ferrite slug threaded into the coil tunes inductance over a small range.
Stray (parasitic) capacitance from PCB traces, component leads, and interwinding capacitance adds to the intended capacitance C, lowering the actual resonant frequency. At high frequencies (MHz range), strays of a few picofarads can shift f₀ significantly. Minimize by shortening leads, using ground planes judiciously, and including stray capacitance in the design calculation.
Microwave cavities resonate at frequencies determined by their physical dimensions (L-C analogy: volume acts as capacitance, current loops as inductance). The resonant frequency for the dominant TE₁₀₁ mode in a rectangular cavity is f = c/(2) × √((m/a)² + (n/b)² + (p/d)²), where a, b, d are dimensions and c is the speed of light. Cavities achieve extremely high Q (10⁴–10⁶) due to negligible resistive losses.
MRI (magnetic resonance imaging) exploits nuclear magnetic resonance. Hydrogen nuclei precess at the Larmor frequency f = γB₀/(2π), proportional to the static magnetic field B₀. For B₀ = 1.5 T (standard MRI), f ≈ 63.8 MHz. RF coils tuned to this frequency excite and detect the precessing nuclei. The LC resonant coil circuit must be precisely tuned to the Larmor frequency for maximum sensitivity.
Parametric resonance occurs when a circuit parameter (L or C) is periodically varied at a frequency related to the natural resonant frequency. Unlike driven resonance (forced at f₀), parametric resonance can build oscillations exponentially without a direct driving signal at f₀. It is exploited in parametric amplifiers (low-noise RF amplifiers using varactors) and is a concern in power systems where periodic voltage variations can excite resonance.
Roboculator Team
The Roboculator Team explains calculations, planning tools, and practical formulas in clear language for real-life situations.
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