The public statement CIV.Main.regularAnnulus #
This module proves the statement CIV.regularAnnulus (lem:aniso:annulus). The annulus assembly
CIV.exists_annulus_bound_wholeBall_conditional_on_serrin takes two inputs beyond the standing
data: the classical form of the equations, supplied by the weak-to-classical bridge
CIV.isClassicalSolutionOn_of_suitable, and Serrin's interior derivative estimate
CIV.Main.serrinInteriorEstimates.
theorem
CIV.Main.regularAnnulus
(q : ℝ)
(u : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Du : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(p : CKN.Foundation.Parabolic.ParabolicPoint → ℝ)
(f : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(hsol : CKN.IsSuitableWeakSolution (CKN.Foundation.Parabolic.vec3Ball 0 1) (Set.Ioo (-1) 0) q u Du p f)
(henergy : GlobalEnergyClass u Du p)
(hu : ContDiffOn ℝ (↑⊤) (fun (z : CKN.Foundation.Parabolic.Vec3 × ℝ) => u z) unitCylinder)
(hp : ContDiffOn ℝ (↑⊤) (fun (z : CKN.Foundation.Parabolic.Vec3 × ℝ) => p z) unitCylinder)
(hf : ContDiffOn ℝ (↑⊤) (fun (z : CKN.Foundation.Parabolic.Vec3 × ℝ) => f z) unitCylinder)
(haxi : IsAxisymmetricOn u unitCylinder)
(hfaxi : IsAxisymmetricOn f unitCylinder)
(hMf : ForceC2Bounded f)
(R₁ R₀ : ℝ)
(hR : 0 ≤ R₁ ∧ R₁ < R₀ ∧ R₀ < 1)
:
∃ (Rm : ℝ) (Rp : ℝ) (t₀ : ℝ),
R₁ < Rm ∧ Rm < Rp ∧ Rp < R₀ ∧ t₀ ∈ Set.Ioo (-1) 0 ∧ (∃ (M : ℝ),
∀ (x : CKN.Foundation.Parabolic.Vec3),
Rm < CKN.Foundation.Parabolic.vec3EuclideanNorm x →
CKN.Foundation.Parabolic.vec3EuclideanNorm x < Rp →
∀ t ∈ Set.Ioo t₀ 0,
∀ (i : Fin 3) (α : Fin 3 → ℕ),
α 0 + α 1 + α 2 ≤ 2 →
|multiPartial (fun (w : CKN.Foundation.Parabolic.ParabolicPoint) => u w i) α (x, t)| ≤ M) ∧ ∀ Rstar ∈ Set.Ioo Rm Rp,
∃ (CΓ : ℝ),
∀ x ∈ CKN.Foundation.Parabolic.vec3Ball 0 Rstar, ∀ t ∈ Set.Ioo t₀ 0, |circulation u (x, t)| ≤ CΓ
The public statement of the regular-annulus lemma lem:aniso:annulus: between any two radii
R₁ < R₀ < 1 there is an annulus and a final time interval on which the derivatives of u of
order at most two are bounded, and on every smaller ball the circulation is bounded.