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Home/Classical Mechanics/Double Pendulum

Double Pendulum

Two coupled rods or masses: a classic chaotic system. Tiny changes in initial angles produce diverging trajectories, illustrating sensitive dependence on initial conditions.

Who it's for: Advanced high school or undergraduate; nonlinear dynamics and chaos demos.

Key terms

  • double pendulum
  • chaos
  • coupled oscillators
  • phase space
  • nonlinearity

Live graphs

Presets

Quick starting points; you can still edit any slider afterward.

Geometry & masses

1.1 m
1.1 m
1 kg
1 kg
9.81 m/s²

Initial angles (from vertical)

65 °
0 °
0 1/s

Both angles are measured from the downward vertical. Motion is integrated with RK4; energy may drift slightly without damping.

Shortcuts

  • •Space — start / pause / resume
  • •R — reset to slider initial conditions

Measured values

KE0.000J
PE0.000J
E total0.000J
ΔE vs start0.0000J
ω₁0.000rad/s
ω₂0.000rad/s

How it works

A classic chaotic system: two point masses on massless rods. Tiny changes in initial angles produce wildly different trajectories. RK4 integration with optional light damping keeps long runs stable.

Key equations

Coupled nonlinear ODEs for θ₁(t), θ₂(t); see standard references for explicit θ¨₁, θ¨₂ (Wikipedia: double pendulum).
E = T + V with T from rod-end velocities and V = −m₁gL₁cos θ₁ − m₂g(L₁cos θ₁ + L₂cos θ₂) + const.

Frequently asked questions

Why is the motion chaotic?
The system is nonlinear and has more than one degree of freedom with coupling, so most initial conditions lead to long-term behavior that is extremely sensitive to small perturbations.