MODEL NOTE
Continuous time becomes a readable section.
The state is (θ1, θ2, ω1, ω2). The fixed RK4 samples are continuous-time states; only the upward crossings of θ2 = 0 mod 2π are placed on the section plot.
OBSERVATION CHAMBER / ACTIVE
Observe a continuous-time double pendulum through a deterministic Poincaré section and compare regular-island and chaotic-sea candidates without claiming a formal chaos proof.
01 / OBSERVE THE SECTION
ROUTE 86 / DYNAMICS / POINCARÉ SECTION
The numeric Poincaré section and energy readouts remain available below.
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Section contract θ2 = 0 mod 2π with an upward crossing ω2 > 0. The crossing state is found by linear interpolation between fixed RK4 samples.
The left plot shows (wrap(θ1), ω1) section points. The right panel shows the same continuous state. A finite pattern is a candidate only; it is not a formal Lyapunov result or a proof of chaos.
03 / READ THE INVARIANTS
04 / CHECK THE NUMERICS
No report yet.
A regular island, mixed layer, or chaotic-sea pattern is a finite observation candidate. This page does not calculate a formal Lyapunov exponent and does not claim a proof of chaos.
MODEL NOTE
The state is (θ1, θ2, ω1, ω2). The fixed RK4 samples are continuous-time states; only the upward crossings of θ2 = 0 mod 2π are placed on the section plot.
SECTION NOTE
Only an upward crossing with ω2 > 0 is accepted. The plotted point uses linear interpolation between the previous and next fixed samples, then wraps θ1 to [−π, π).
LIMIT NOTE
Regular islands, mixed layers, and chaotic-sea candidates can appear in a finite window. Energy drift and finite guards are shown so that numerical consistency is visible beside the pattern.
FORMULA / CONTRACT
dθ1/dt = ω1, dθ2/dt = ω2
dω1/dt = [−g(2m1+m2)sinθ1 − m2g sin(θ1−2θ2) − 2m2sinδ(l2ω22 + l1ω12cosδ)] / [l1(2m1+m2−m2cos2δ)]
dω2/dt = 2sinδ[l1ω12(m1+m2) + g(m1+m2)cosθ1 + l2m2ω22cosδ] / [l2(2m1+m2−m2cos2δ)]
E(t) = ½(m1+m2)l12ω12 + ½m2l22ω22 + m2l1l2ω1ω2cosδ − (m1+m2)gl1cosθ1 − m2gl2cosθ2
Here δ = θ1 − θ2, angles are measured from the downward vertical. The default REGULAR preset starts at Einit = −28.929 J; the downward equilibrium reference is Eeq = −29.430 J for m1 = m2 = 1 kg, L = 1 m, g = 9.81 m/s². The drift readout uses Einit, not Eeq.
HOW TO OBSERVE
This observatory runs a deterministic, browser-local continuous-time double-pendulum model. Angles, calculations, section points, reports, and images stay local. It does not measure visitors or a real pendulum.
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