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LeanPool.CaffarelliKohnNirenberg.Leray.RegEquicontinuity

Reg Equicontinuity #

Supporting estimates for the Navier–Stokes development.

theorem CKN.Leray.regEqui_pairing_equation_ibp (f : Fin 3 → Foundation.Parabolic.Vec3 → ℝ) (g : Fin 3 → Fin 3 → Foundation.Parabolic.Vec3 → ℝ) (h : Fin 3 → Fin 3 → Fin 3 → Foundation.Parabolic.Vec3 → ℝ) (P : Foundation.Parabolic.Vec3 → ℝ) (q J F w : Fin 3 → Foundation.Parabolic.Vec3 → ℝ) (hf : ∀ (i : Fin 3), Continuous (f i)) (hfdiff : ∀ (i : Fin 3) (x : Foundation.Parabolic.Vec3), DifferentiableAt ℝ (f i) x) (hfd : ∀ (i j : Fin 3) (x : Foundation.Parabolic.Vec3), (fderiv ℝ (f i) x) (basisVec j) = g i j x) (hg : ∀ (i j : Fin 3), Continuous (g i j)) (hgdiff : ∀ (i j : Fin 3) (x : Foundation.Parabolic.Vec3), DifferentiableAt ℝ (g i j) x) (hgd : ∀ (i j k : Fin 3) (x : Foundation.Parabolic.Vec3), (fderiv ℝ (g i j) x) (basisVec k) = h i j k x) (hh : ∀ (i j k : Fin 3), Continuous (h i j k)) (hP : Continuous P) (hPdiff : ∀ (x : Foundation.Parabolic.Vec3), DifferentiableAt ℝ P x) (hPd : ∀ (i : Fin 3) (x : Foundation.Parabolic.Vec3), (fderiv ℝ P x) (basisVec i) = q i x) (hq : ∀ (i : Fin 3), Continuous (q i)) (hJ : ∀ (j : Fin 3), ContDiff ℝ 1 (J j)) (hdivJ : ∀ (x : Foundation.Parabolic.Vec3), ∑ j : Fin 3, (fderiv ℝ (J j) x) (basisVec j) = 0) (hF : ∀ (i : Fin 3) (x : Foundation.Parabolic.Vec3), F i x = ∑ j : Fin 3, h i j j x - ∑ j : Fin 3, J j x * g i j x - q i x) (hw : ∀ (i : Fin 3), ContDiff ℝ (↑⊤) (w i)) (hwc : ∀ (i : Fin 3), HasCompactSupport (w i)) :
∫ (x : Foundation.Parabolic.Vec3), ∑ i : Fin 3, F i x * w i x = (∫ (x : Foundation.Parabolic.Vec3), ∑ i : Fin 3, ∑ j : Fin 3, (f i x * spatialDeriv (spatialDeriv (w i) j) j x + f i x * J j x * spatialDeriv (w i) j x)) + ∫ (x : Foundation.Parabolic.Vec3), P x * ∑ i : Fin 3, spatialDeriv (w i) i x

The exponent-two pressure slice formula identifies the pressure with the space-time Riesz representative at exponent five-thirds whenever the regularized tensor has its global five-thirds bound. This is the pressure input to lem:reg-equicontinuity.