Proof IV of VII

Contact Geometry

Maximal non-integrability and the Hill coefficient
The contact form α = dz − r²dθ on the dm³ manifold is maximally non-integrable at the fold. This geometric constraint fixes a universal sigmoid Hill coefficient n ≈ 3.64 — making HVEH performance predictable across all rainfall intensities.

The contact form α = dz − r²dθ defines a plane field on the 3-dimensional dm³ manifold that is maximally non-integrable: no surface exists everywhere tangent to the planes defined by ker(α). This is what prevents the helical flow from collapsing into a planar, non-rotating state.

The Reeb vector field R = ∂z, defined by ι_R α = 1 and ι_R dα = 0, generates the persistent helical motion. Every orbit of R is a Legendrian curve — the flow follows the contact geometry inevitably, without external forcing.

The transverse Lyapunov exponent μ_max = −2 quantifies how strongly perturbations away from the limit cycle Γ are damped. Combined with the fold geometry at r*, it fixes the sigmoid Hill coefficient n ≈ 3.64 — steep enough to act as a flood gate, shallow enough to avoid cavitation.

The basin hierarchy ε₀=1/3 < r*≈0.776 < κ*≈0.882 < 1 demarcates three nested zones: the inner laminar core, the transition annulus, and the outer turbulent boundary. All three are determined by the contact geometry alone.

Key relations
Contact formα = dz − r² dθ
Non-integrabilityα ∧ dα ≠ 0 everywhere
Reeb fieldR = ∂z generates persistent rotation
Lyapunov exponentμ_max = −2
Hill coefficientn ≈ 3.64
Basin hierarchyε₀=1/3 < r*≈0.776 < κ*≈0.882 < 1
κ* ≈ 0.882 outer boundary r* ≈ 0.776 transition ε₀ = 1/3 laminar core R = ∂z ker(α) contact plane μ_max = −2 · T* = 2π · n ≈ 3.64 α = dz − r² dθ on dm³
Engineering consequence
The Hill coefficient n ≈ 3.64 is universal across all HVEH module sizes — set by the geometry of the contact manifold, not module dimensions. A small outfall module and a large harbor module have the same transition sharpness, shifted only in absolute flow rate.