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Electricity · Physics

LC Oscillations 3D Simulation: LC & LCR Circuits

A charged capacitor joined to a coil, in 3D: charge drains off the plates, current runs round the wire and the coil's magnetic field swells, then it all swings back. Energy bars show ½CV² and ½Li² trading places; a mass on a spring moves in step beside it; and resistance damps it out.

Interactive virtual lab · no download · works on phones and laptops

Chapter
Alternating Current
For
Class 12 · JEE · NEET
Time
~20 min

LC Oscillations is a Pro simulation

Pro opens all 152 virtual labs — 693 simulations with guides and quizzes.

How to use it

  1. 1Pick a module from the list (3); set your level at the top right for more controls.
  2. 2Change L, C and the starting charge; the stage runs one cycle every 2.5 s on its own.
  3. 3Use Predict before you look, then Derive, Questions, Practise and Compare.

What to notice

  • Charge and current are a quarter cycle apart: the current peaks as the plates empty.
  • Energy swings between the capacitor's electric field and the coil's magnetic field; the total stays Q₀²/2C.
  • f = 1/(2π√(LC)): four times the capacitance doubles the period.
  • Resistance damps it; at R = 2√(L/C) the charge returns without swinging.

For teachers

A ready-made teaching kit comes with this lab

  • Lesson plan

    25 min, 4 steps

  • Ask the class

    4 questions with answers

  • Quick quiz

    6 questions, printable

  • Key formulas

    5 formulas

About the LC Oscillations simulation

An LC circuit is a capacitor and a coil joined in a loop, and it is the electrical twin of a mass on a spring. This 3D LC oscillations simulation charges the capacitor and closes the loop: charge drains off the plates through the coil, the current builds and the coil's magnetic field swells, and when the capacitor is empty the coil keeps the current going and charges it the other way round. The stage runs by itself, one cycle every two and a half seconds, with the energy bars for ½CV² and ½Li² trading places as it goes.

The second module puts a block on a spring beside the circuit, moving in step: charge is displacement, current is velocity, inductance is mass and 1/C is stiffness. The third adds resistance, which heats up and drains the energy each cycle, so the oscillation dies inside an envelope e^(−Rt/2L) — and at the critical resistance 2√(L/C) the charge simply creeps back to zero without swinging. Each module has a prediction, a derivation, exam-style questions with hints and fresh numericals.

Also covers: lc circuit, lc oscillation, oscillating circuit, tank circuit, energy in capacitor and inductor, electric and magnetic energy, natural frequency 1/2π√lc, lcr circuit, damped oscillation, critical damping, critical resistance, quality factor, mass spring analogy, class 12 alternating current, jee lc oscillation.

Frequently asked questions

What is the frequency of an LC circuit?

f = 1/(2π√(LC)). With L = 10 mH and C = 10 µF, √(LC) = 3.16 × 10⁻⁴ s, so f ≈ 503 Hz. Making C four times larger halves the frequency (doubles the period), because f depends on the square root.

When is the current largest in an LC circuit?

At the instant the capacitor's charge is zero. The total energy q²/2C + ½Li² is fixed, so when q = 0 all of it is in the coil and i is at its peak, I₀ = Q₀ω₀. Charge and current are a quarter cycle apart.

Why do the oscillations in a real LC circuit die out?

Real wires and coils have resistance, and the current heats them: energy i²R per second leaves the circuit. The oscillation decays as e^(−Rt/2L). Above R = 2√(L/C) it does not oscillate at all.

How is an LC circuit like a mass on a spring?

Both obey the same equation: Lq̈ + q/C = 0 and mẍ + kx = 0. Inductance plays mass (it resists changes in current as mass resists changes in velocity) and 1/C plays the spring constant.