Helical Attractors on Contact 3-Manifolds
and the Inner Basin Boundary r*

LAW3M · Law of Geometric Space Dynamics · Technical Brief · June 2026
Pablo Nogueira Grossi · G6 LLC
Newark NJ USA
ORCID 0009-0000-6496-2186
doi:10.5281/zenodo.19117399
System — (ℝ³, α = dz − r²dθ) · ε = 2
ṙ = r(1 − r²) + 2(r−1)e⁻ᶻ
θ̇ = 1
ż = r² − 2(r−1)²e⁻ᶻ
Contact condition: dz = r²dθ (lift = angular momentum)
Attractor: Γ = {r=1, θ̇=1, ż=1} · Lyapunov μ = −2

The contact condition α = 0 is a geometric identity: vertical lift is proportional to r² times angular velocity. The disk cross-section, horizontal hover, and lift scaling are consequences of the contact form — not tunable parameters.

Certified result — DOP853 · rtol=10⁻¹² · bisection tol=10⁻⁷
r* = 0.77594059
Inner basin boundary · 7 sig. figs. · <2 min on any IEEE-754 platform
ε₀=1/3 < 2/3 < r*=0.77594 < κ*=√(7/9) < 1

r* is a Whitney A₁ fold singularity — the point where two qualitatively different convergence paths merge onto the attractor. Below r*, the trajectory escapes irreversibly. The fold is not a numerical artifact; it is a topological feature of the contact manifold.

Saddle Geometry — Closed-Form Results (Theorems B.1–B.5)

Theorem B.1 (Saddle cubic). The saddle r-coordinate is the unique root in (0,1) of r³ − r² − 2r + 1 = 0, equal to rs = 2 cos(3π/7) ≈ 0.4450.

Theorem B.2 (Fundamental identity). (1 + rs − rs²)² = 2 − rs.

Theorem B.3 (Trace identity). tr(J)|saddle = 1 + rs − rs² = √(2 − rs) = 2 cos(2π/7).

Theorem B.4 (J22 exact). J22|saddle = rs².

Theorem B.5 (Eigenvalue formula). λ± = cos(2π/7) ± ½√(32rs² + 15rs − 10); numerically λ+ ≈ 1.1097 (unstable), λ ≈ −0.2443 (saddle).

The saddle rs is now analytically resolved. The basin boundary r* ≈ 0.775940575502295 is a distinct, transcendental object — the Whitney A₁ fold threshold — and remains an open analytic problem.


Three-Disk Engine — Physical Configuration
VIEW FROM BELOW — THREE PLASMA ARMS r* = 0.776 corona Γ: r=1 α = dz − r²dθ = 0 three arms · 120° · Newgrange c.3200 BCE · same structure SIDE VIEW — HELICAL ATTRACTOR z (lift) r r* 1 escape inner basin outer basin Γ: r=1, ż=1 Whitney A₁ fold at r* ż = r² → lift ∝ (angular velocity)²
Three Industry Vectors
Vector I

Electric Powertrains
BMW · Mercedes-Benz EV

A permanent magnet synchronous motor (PMSM) operates in the same (r, θ, z) geometry as the LAW3M system. The dq-frame decomposition is the contact manifold in engineering notation.

BMW eDrive Mercedes EQS PMSM field weakening
Whitney fold at r* MTPA → field-weakening knee
ż = r² (lift ∝ ω²) Back-EMF ∝ ω² above base speed
Three disks at 120° Three-phase stator U/V/W
Escape: r < r* Demagnetisation / stall

The certified r* = 0.77594 gives a geometry-native definition of the efficiency boundary — independent of material constants, derived from the contact structure alone.

Vector II

Autonomous Truck Control
Mercedes eActros · SAE L4

A truck-trailer system has a non-holonomic steering constraint — the trailer's velocity must be tangent to its own axis at the hitch. This constraint is a contact condition on the configuration space (x, y, θ_truck, φ_hitch).

eActros LongHaul SAE Level 4 jackknife path planning
α = dz − r²dθ = 0 Trailer tangency constraint
Attractor Γ Reference lane / path
Whitney fold at r* Critical hitch angle: jackknife onset
Escape: r < r* Jackknife — irreversible

The basin boundary r* gives a geometry-native safety margin for autonomous steering controllers: a hard boundary derivable analytically, not empirically tuned. Relevant for ISO 11270 lane-keeping and EU truck platooning standards.

Vector III

Plasma & Aerospace Propulsion
SpaceX · PPPL · NASA

Three counter-rotating disks at 120° — shown in the schematic above — are the minimal physical realisation of the contact manifold. The disk cross-section, hover axis, and lift scaling ż = r² follow from the contact form alone. At r = r* = 0.77594, the coupling term reaches ionisation threshold: plasma corona discharge at the Whitney fold.

three-disk engine corona at r* helical confinement toroidal attractor
Three disks at 120° Triple-helical / stellarator coil
Whitney fold at r* Ionisation / corona onset
ż = r² (axial lift) Axial pressure ∝ ω² — hover
Escape: r < r* Plasma quench / arc extinction

The disk shape, horizontal hover, and plasma corona are all consequences of the contact form α = dz − r²dθ. None require aerodynamics. The geometry selects them.


Reproducibility & Open Access

All results derive from certify_rstar.py — a single MIT-licensed Python script (NumPy + SciPy only). No randomness, no platform tuning. Running time <2 min. Expected output identical on any IEEE-754 double-precision system. Formal mechanisation in Lean 4 is in progress at github.com/TOTOGT/AXLE; open theorems are flagged as sorry with explicit statements — no hidden assumptions.

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