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LeanPool.EscauriazaSereginSverak.Endpoint.VorticityChain

The div–curl chain at a fixed time #

At a fixed time, three applications of the div–curl estimate and one of the H² to L∞ embedding bound the smooth approximations of the first, second and third derivatives of the velocity, and the gradient pointwise, by the vorticity and its derivatives (the velocity levels of thm:vorticity-regularity).

theorem ESS.vorticity_sum_rotate (f : Fin 3 → Fin 3 → Fin 3 → ℝ) :
∑ j : Fin 3, ∑ k : Fin 3, ∑ l : Fin 3, f l j k = ∑ l : Fin 3, ∑ j : Fin 3, ∑ k : Fin 3, f l j k

Rotating the order of a triple sum.

theorem ESS.vorticityChain {ρ : ℝ} (hρ : 4 / 64 < ρ) :
∃ (C : ℝ), 0 ≤ C ∧ ∀ (x₀ : CKN.Foundation.Parabolic.Vec3) (t : ℝ) (U w : Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ) (G Ω1 : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ) (D2 Ω2 : Fin 3 → Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ), (∀ (i : Fin 3), ContDiff ℝ (↑⊤) (U i)) → (∀ (i j : Fin 3), ContDiff ℝ (↑⊤) (G i j)) → (∀ (i j k : Fin 3), ContDiff ℝ (↑⊤) (D2 i j k)) → (∀ (i : Fin 3), Continuous (w i)) → (∀ (i j : Fin 3), Continuous (Ω1 i j)) → (∀ (i j k : Fin 3), Continuous (Ω2 i j k)) → (∀ x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∑ i : Fin 3, CKN.spatialPartial (U i) i (x, t) = 0) → (∀ x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∀ (i k : Fin 3), CKN.spatialPartial (U k) i (x, t) - CKN.spatialPartial (U i) k (x, t) = vorticityAntisym (fun (l : Fin 3) => w l (x, t)) i k) → (∀ x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∀ (i j : Fin 3), CKN.spatialPartial (U i) j (x, t) = G i j (x, t)) → (∀ x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∀ (m : Fin 3), ∑ i : Fin 3, CKN.spatialPartial (G i m) i (x, t) = 0) → (∀ x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∀ (m i k : Fin 3), CKN.spatialPartial (G k m) i (x, t) - CKN.spatialPartial (G i m) k (x, t) = vorticityAntisym (fun (l : Fin 3) => Ω1 l m (x, t)) i k) → (∀ x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∀ (i j k : Fin 3), CKN.spatialPartial (G i j) k (x, t) = D2 i j k (x, t)) → (∀ x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∀ (j k : Fin 3), ∑ i : Fin 3, CKN.spatialPartial (D2 i j k) i (x, t) = 0) → (∀ x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∀ (j k i c : Fin 3), CKN.spatialPartial (D2 c j k) i (x, t) - CKN.spatialPartial (D2 i j k) c (x, t) = vorticityAntisym (fun (l : Fin 3) => Ω2 l j k (x, t)) i c) → ∫ (x : CKN.Foundation.Parabolic.Vec3) in CKN.Foundation.Parabolic.vec3Ball x₀ (ρ - 1 / 64), ∑ i : Fin 3, ∑ j : Fin 3, G i j (x, t) ^ 2 ≤ C * ∫ (x : CKN.Foundation.Parabolic.Vec3) in CKN.Foundation.Parabolic.vec3Ball x₀ ρ, ∑ l : Fin 3, w l (x, t) ^ 2 + ∑ i : Fin 3, U i (x, t) ^ 2 ∧ ∫ (x : CKN.Foundation.Parabolic.Vec3) in CKN.Foundation.Parabolic.vec3Ball x₀ (ρ - 2 / 64), ∑ i : Fin 3, ∑ j : Fin 3, ∑ k : Fin 3, D2 i j k (x, t) ^ 2 ≤ C * ∫ (x : CKN.Foundation.Parabolic.Vec3) in CKN.Foundation.Parabolic.vec3Ball x₀ (ρ - 1 / 64), ∑ l : Fin 3, ∑ m : Fin 3, Ω1 l m (x, t) ^ 2 + ∑ i : Fin 3, ∑ j : Fin 3, G i j (x, t) ^ 2 ∧ ∫ (x : CKN.Foundation.Parabolic.Vec3) in CKN.Foundation.Parabolic.vec3Ball x₀ (ρ - 3 / 64), ∑ i : Fin 3, ∑ j : Fin 3, ∑ k : Fin 3, ∑ c : Fin 3, CKN.spatialPartial (D2 i j k) c (x, t) ^ 2 ≤ C * ∫ (x : CKN.Foundation.Parabolic.Vec3) in CKN.Foundation.Parabolic.vec3Ball x₀ (ρ - 2 / 64), ∑ l : Fin 3, ∑ j : Fin 3, ∑ k : Fin 3, Ω2 l j k (x, t) ^ 2 + ∑ i : Fin 3, ∑ j : Fin 3, ∑ k : Fin 3, D2 i j k (x, t) ^ 2 ∧ ∀ (x : CKN.Foundation.Parabolic.Vec3), CKN.Foundation.Parabolic.vec3EuclideanNorm (x - x₀) ≤ ρ - 4 / 64 → ∀ (i j : Fin 3), G i j (x, t) ^ 2 ≤ C * ∫ (y : CKN.Foundation.Parabolic.Vec3) in CKN.Foundation.Parabolic.vec3Ball x₀ (ρ - 3 / 64), G i j (y, t) ^ 2 + ∑ k : Fin 3, D2 i j k (y, t) ^ 2 + ∑ k : Fin 3, ∑ c : Fin 3, CKN.spatialPartial (D2 i j k) c (y, t) ^ 2

The div–curl chain at a fixed time, on the balls of radii ρ, ρ - 1/64, …, ρ - 4/64.