Pendulum Waves — Emergent Patterns from SHM

Simple pendulums tuned to different frequencies spontaneously produce travelling waves, standing waves, and synchrony.

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N: 15

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15
0.70
60

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The Physics of Pendulum Waves

A pendulum wave apparatus consists of N pendulums with carefully chosen lengths. The lengths are not arbitrary — each pendulum k is designed to complete exactly (nmin + k) oscillations in one cycle time T. Because each pendulum executes simple harmonic motion (SHM) independently, their collective motion sweeps through a sequence of beautiful, predictable patterns over time.

Design equations:
Pendulum k completes nMin + k oscillations in T seconds.
Period: T_k = T / (nMin + k)
Length: L_k = g · T_k² / (4π²) = g·T² / (4π²·(nMin+k)²)
Position: x_k(t) = A · sin(2π·(nMin+k)·t / T)

Synchrony (t = 0, T)

All pendulums start in phase. Reoccurs exactly at every multiple of T — typically 60 seconds.

Travelling Wave (t ≈ T/4)

Phase differences grow linearly across pendulums, producing an apparent wave sweeping left to right.

Standing Wave (t ≈ T/2)

At the half-cycle, even and odd pendulums are in antiphase, producing a symmetric nodal pattern.

Serpent / Diamond

Intermediate times reveal complex multi-node shapes — the number of apparent groups equals the time fraction denominator.

Pattern Sequence (Classic 15, T=60s)

TimePatternDescription
0 sSynchronyAll 15 bobs aligned — a single cluster
~7.5 s8 groupsBobs arrange into 8 visible clusters
~10 s6 groups6 distinct groups visible
~15 sTravelling waveSmooth phase ramp — apparent rightward motion
~20 s3 groupsThree clusters oscillate together
~30 sStanding waveTwo antiphase halves — 7–8 node pattern
~45 sTravelling waveReversed — apparent leftward motion
60 sSynchronyAll pendulums return to exact alignment

Why It Works: Beats and Phase

The key insight is that adjacent pendulums differ by exactly one oscillation per cycle. The relative frequency between pendulum k and k+1 is Δf = 1/T — meaning they drift apart at a constant rate and re-align after exactly T seconds. This predictability is why the patterns are so strikingly regular and reproducible.

The phenomenon is related to quantum revivals in physics: a wavepacket spreads over time due to dispersion, then re-forms (revives) when the phases realign — a direct analogue of all pendulums returning to synchrony at t = T. Similarly, the intermediate patterns correspond to fractional revivals where subsets of the pendulums phase-align.

Number of groups at time t: The apparent number of clusters equals gcd(nMin, floor(t·N/T)) approximately — the visible grouping is determined by how many pendulums have completed an integer number of half-cycles relative to each other.

The Harvard Demonstration

The most famous physical implementation was built by the Harvard Natural Sciences Lecture Demonstrations group. Their apparatus uses 15 pendulums with lengths calculated to complete 51 through 65 oscillations in 60 seconds — the same parameters used in the Classic 15 preset here. The video of this demonstration has been viewed millions of times online and introduced wave physics to a generation of students. The apparatus requires precise machining: the longest pendulum is about 2.4 m and the shortest about 1.1 m.

Frequently Asked Questions

Why do the periods start with 51 swings?
The choice of nmin = 51 is practical rather than fundamental. With 15 pendulums completing 51–65 oscillations in 60 seconds, the pendulum lengths are in a convenient range (roughly 1–2.5 m) for a table-top demonstration. Starting at 51 rather than 1 makes the lengths much closer to each other, so the apparatus can hang neatly in a row without extremely different string lengths.
Does air resistance spoil the pattern?
In a real apparatus, yes — air resistance damps the swing amplitude, and the pendulums of different lengths have slightly different decay rates. This means the patterns gradually fade over many cycles. The Harvard apparatus uses carefully shaped, aerodynamic bobs and light strong strings to minimise damping, allowing several clean repeat cycles. This simulation uses undamped SHM, so patterns repeat perfectly indefinitely.
What is the connection to quantum mechanics?
The phenomenon of all pendulums returning to synchrony at t = T is directly analogous to quantum revivals. In a quantum system with equally spaced energy levels (like an infinite square well or a Rydberg atom), a localised wave packet disperses and reforms periodically. The revival time Trev = 2π/Δω (where Δω is the frequency spacing) corresponds exactly to the cycle time T in the pendulum wave — the same maths governs both systems.
Can I add more than 25 pendulums?
The simulator caps at 25 for visual clarity — with too many pendulums the individual bobs overlap. Mathematically there is no limit; a continuous limit where N → ∞ produces a perfectly smooth sinusoidal travelling wave at all times (the individual bobs become a continuum string), and the discrete clustering patterns disappear. The finite-N patterns are therefore a distinctly discrete-system effect — another parallel to quantum systems.