Lissajous Curves & Parametric Equations
Trace the elegant figures produced by two coupled sinusoidal oscillations at right angles. Explore how frequency ratios encode musical intervals, watch the phase shift morph the shape continuously, and read the x and y motions from the oscilloscope side panels.
Space pause C clear S sweep 1–5 presets
What Are Lissajous Curves?
A Lissajous curve (pronounced lee-SAH-zhoo) is the graph of a system of parametric equations:
y(t) = B · sin(b·t)
where a and b are the angular frequencies along the x and y axes, δ is the phase offset, and A, B are amplitudes. They were first analytically studied by American mathematician Nathaniel Bowditch (1815) — hence the alternative name Bowditch curves — and later recreated optically by French physicist Jules Antoine Lissajous (1857) who used tuning forks and mirrors to project the figures in light.
Closed vs Open Curves
When a:b is a rational number (ratio of two integers), the curve is closed — it repeats exactly after a period T = 2π / gcd(a,b). When a:b is irrational, the curve is open and eventually fills the entire A×B rectangle, never exactly retracing its path.
Counting Lobes
For a ratio a:b in lowest terms, the Lissajous curve crosses the vertical bounding line 2b times and the horizontal bounding line 2a times. The number of interior lobes is (a−1)(b−1) + (a−1)/2 + (b−1)/2 for odd sums, giving a quick visual check.
Phase Shift δ
The phase shift rotates and deforms the figure. For 1:1 ratio, δ = 0 gives a diagonal line, δ = π/4 gives a tilted ellipse, δ = π/2 gives a circle. The Sweep Phase button animates this transition, used in physics labs to demonstrate SHM superposition.
Musical Intervals
Frequency ratios map to musical intervals. 1:2 = octave, 2:3 = perfect fifth, 3:4 = perfect fourth, 4:5 = major third. This connection between geometry and harmony fascinated 19th-century scientists and inspired Helmholtz's work on consonance.
Common Frequency Ratios
| Ratio a:b | Phase δ = π/2 | Musical Interval | Lobes |
|---|---|---|---|
| 1:1 | Circle or ellipse | Unison | 1 |
| 1:2 | Figure-8 (∞) | Octave | 2 |
| 1:3 | Triple loop | Octave + fifth | 3 |
| 2:3 | Two humps / three loops | Perfect fifth | 6 |
| 3:4 | Complex interlaced loops | Perfect fourth | 12 |
| 4:5 | Dense interlaced figure | Major third | 20 |
| 5:6 | Very dense figure | Minor third | 30 |
The Oscilloscope Connection
Engineers use X-Y mode on an oscilloscope to compare two sinusoidal signals. If one signal drives the x-deflection plates and another the y-deflection plates, the resulting trace is exactly a Lissajous figure. The shape reveals the frequency ratio and phase difference between the signals:
- A circle → same frequency, δ = π/2 (90° phase difference)
- A diagonal line → same frequency, δ = 0 (in phase)
- A figure-eight → 1:2 frequency ratio
- Phase difference formula:
sin(δ) = Y₀ / Y_max, where Y₀ is the y-intercept
The side oscilloscope panels in this simulator show the individual sinusoidal projections that combine to produce the Lissajous figure — exactly what you'd measure on two separate oscilloscope channels.
Physics: Coupled Harmonic Oscillators
A Blackburn pendulum consists of a weight suspended from two pivots at right angles. By setting the pendulum lengths to achieve integer frequency ratios, the bob traces a perfect Lissajous figure in sand. For a pendulum of length L, the natural frequency is f = (1/2π)√(g/L). To get a 2:3 ratio, the y-axis pendulum must be 9/4 times longer than the x-axis pendulum, since f ∝ 1/√L.
Period of a Closed Lissajous Curve
A closed Lissajous curve with frequency ratio a:b (in lowest terms) completes one full cycle in time:
For a=3, b=2: T = 2π/1 = 2π. For a=4, b=6: first reduce to 2:3, T = 2π/gcd(2,3) = 2π. The HUD 'Period' readout shows this value in radians.
Applications in Science & Engineering
⚡ Electrical Engineering
Phase measurement, frequency ratio verification, signal analysis using oscilloscopes in X-Y mode. Standard technique in electronics labs and circuit testing.
🌍 Seismology
Two-component seismograph records produce Lissajous-like particle motion plots revealing the polarisation of seismic waves and source direction.
🚀 Space Mechanics
Spacecraft near Lagrange points (SOHO at L1, JWST at L2) follow three-dimensional Lissajous orbits — halo orbits with incommensurate frequencies in each plane.
🎵 Music Technology
Oscilloscope visualisers in synthesisers display Lissajous figures from stereo signals, letting musicians visualise stereo phase and harmonic relationships in real time.
Related Simulations
Fourier Series
Decompose any periodic wave into sinusoidal components — the building blocks of Lissajous motion.
Spring-Mass System
Coupled spring oscillators in 2D trace Lissajous-like paths when their natural frequencies form integer ratios.
Wave Superposition
Add sinusoidal waves and observe interference — the 1D cousin of the 2D Lissajous superposition.
Pendulum
The simple pendulum's small-angle motion is the sinusoidal component that Lissajous figures are built from.
📖 Deep Dive Article
Read the full educational article: Lissajous Curves & Parametric Equations: The Mathematics of Coupled Oscillations — covering history, Bowditch's original analysis, musical intervals, oscilloscope phase measurement, and Lissajous knots in 3D.