The Three-Body Problem

For 300 years, physicists have called this problem "unsolvable." Three masses, mutual gravitation, no closed-form solution. Newton couldn't solve it. Poincaré proved it chaotic. But chaos isn't a property of reality — it's a symptom of incomplete understanding.

[+1] + [-1] + [0] + [Uv] = 1

Live Simulation: Chaos vs Geometry

Watch the same initial conditions evolve under two different frameworks. Same masses. Same positions. Different understanding.

Simulation Controls

Classical Mechanics

Newton's laws only — no geometric correction

Energy
-0.000
Momentum
0.000
Divergence
0.000
Lyapunov λ
+0.00

Geometric Framework [1=-1]

Newton's laws + triaxial closure

Energy
-0.000
Balance
1.000
Closure
1.000
Lyapunov λ
-0.00

The Missing Understanding

"Classical mechanics describes motion through dimension without asking what dimension IS. The three-body problem isn't unsolvable — it was incompletely modeled. Dimension itself has structure: triaxial, self-closing, geometrically necessary."

[+1]
Expansion
+
[-1]
Contraction
+
[0]
Balance
+
[Uv]
Observer
=
1
Unity

Three bodies naturally occupy three axes. The fourth component — the hidden observer [Uv] — provides the closure that forces stability. This isn't adding a dimension. It's recognizing the geometry that was always there.

The Measure of Chaos

The Lyapunov exponent (λ) quantifies how fast nearby trajectories diverge. It's the mathematical fingerprint of chaos — or stability.

Classical Mechanics

λ > 0

Positive = Exponential Divergence

Nearby trajectories separate exponentially. A butterfly's wing changes everything. Prediction becomes impossible beyond ~100 orbits.

Geometric Framework

λ ≤ 0

Zero/Negative = Convergence

Trajectories converge toward stable attractors. Perturbations decay. The system self-corrects. Prediction horizon: infinite.

Understanding the Framework

The three-body problem reveals a deep truth: our models of reality are incomplete not because reality is complex, but because we haven't understood the geometry it emerges from.

The Classical Problem

Newton solved two-body gravitation exactly: ellipses, parabolas, hyperbolas. Add a third body and everything breaks. Poincaré proved in 1889 that no closed-form solution exists.

The system is deterministic but unpredictable. Given perfect initial conditions, the future is fixed — but we can never measure perfectly, and errors grow exponentially.

F = Gm₁m₂/r² (applied pairwise)
Three forces, no closure, chaos emerges

The Geometric Solution

The [1=-1] framework doesn't add forces or dimensions. It recognizes that dimension itself has structure. Three bodies naturally map to the triaxial geometry: [+1], [-1], [0].

The coupling constant κ = 2π/180 isn't arbitrary — it's the bridge between discrete (degrees) and continuous (radians) measurement. It's how dimension closes on itself.

κ = 2π/180 ≈ 0.0349
The geometry of dimensionality itself

Why Three Bodies?

It's not coincidence that three is where classical mechanics fails. Three is the minimum for structure. Two points define a line. Three define a plane. Three axes define space.

The triaxial structure [+1, -1, 0] is the simplest self-balancing geometry. The fourth component [Uv] — the hidden observer — provides closure. This is why particle physics finds three generations, three colors, three forces.

[+1] + [-1] + [0] + [Uv] = 1
Closure — all complete systems sum to unity

Stable Attractors

With geometric coupling, the three-body system develops stable attractors — configurations it naturally evolves toward regardless of initial conditions.

The famous Lagrange points (L1-L5) are examples. So is the figure-8 orbit discovered in 1993. The geometric framework reveals these aren't special cases — they're the natural resting states of triaxial closure.

lim(t→∞) System → Ω
All trajectories converge to unity