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LC oscillations

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Charge in an LC circuit oscillates like a mass on a spring.

Key relationω = 1/√(LC)

In an LC circuit charge oscillates at ω = 1/√(LC), swapping energy between the capacitor's electric field and the inductor's magnetic field.

Worked example

L = 1 mH, C = 1 μF: f ≈ 5 kHz.

Common mistake

Resistance damps it.

In more detail

An LC circuit has an inductor and capacitor that exchange energy, oscillating at ω = 1/sqrt(LC). Electrical energy swaps between the capacitor's electric field and the inductor's magnetic field.

Real-world uses

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Frequently asked questions

What is the frequency?

ω equals 1 divided by the square root of LC.

What is the analogy?

The capacitor plays the role of a spring and the inductor the role of mass.

Does an LC circuit oscillate forever?

Not in practice. Resistance in the circuit damps the oscillation, but a low-resistance circuit oscillates for many cycles.

Related topics in Oscillations & SHM

Resonance · Resonance examples · Amplitude vs frequency curve · Analogy between mechanical and electrical oscillators · Coupled oscillators · Normal modes

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