Documentation

NavierStokes.Geometry.AutoLinearization

def AutoLinearization.vorticityDir (omega_val : Fin 3) :
Fin 3

The Vorticity Direction Field $\xi(x,t) = \frac{\omega(x,t)}{|\omega(x,t)|}$. Defined strongly when $\omega \neq 0$.

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    Enstrophy functional $\mathcal{E}(u) = \sum_k |k \times \hat{u}_k|^2$. This represents the $L^2$ norm of the vorticity.

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      The alignment functional $\beta(u)$ measuring the defect of helicity relative to enstrophy.

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        The Vortex Stretching term $\int \omega \cdot S \omega$ in Fourier space. Technically a convolution, represented here as an integrated interaction functional.

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          Phase Rigidity and Auto-Linearization (Section 3) - Étape 1: Cinématique #

          Instead of a structural hypothesis, we derive the alignment decay from the conservation of the topological invariant $H$ (Helicity). All physical parameters are universally quantified as explicit theorem parameters.

          Cauchy-Schwarz Justification for helicity_bound #

          The hypothesis helicity_bound : beta * omega_norm² ≤ H follows from the integral Cauchy-Schwarz inequality in Fourier space: H = |∫ u·ω| = |∑_k û_k · (ik × û_k)| ≤ ∑_k |û_k|·|k|·|û_k| = ∑_k |k|·|û_k|² ≤ beta · (∑_k |k|²·|û_k|²) = beta · omega_norm² where beta measures the alignment defect (= 1 for perfect alignment).

          theorem AutoLinearization.bound_chain (a b c d : ) (hb : 0 b) (h1 : a b * c) (h2 : c d) :
          a b * d

          Algebraic Cauchy-Schwarz: if a ≤ b·c and c ≤ d, then a ≤ b·d (used to chain the helicity bound with enstrophy).

          Lemme 3.1 : Auto-linéarisation Kinématique (Analytique) The topology forces the alignment coefficient to decay as enstrophy increases. $\beta(u) \le H(u) \cdot \Omega(u)^{-2}$.

          Théorème : Lemme 3.2 (Sub-criticalité Analytique) Helicity conservation forces a sub-linear growth of the stretching term. The cubic growth is reduced by the topological decay of $\beta(u)$.

          Appendix A (sealed form) #

          Localized contradiction is encoded in the global decay estimate by choosing the explicit exponent α = 1.