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LeanPool.CIVAxisymmetric.Analysis.DivCurl

The elliptic identity ‖∇v‖² = ‖curl v‖² + ‖div v‖² #

This file proves the elliptic identity eq:aniso:closure:elliptic of Regularity of asymptotically axisymmetric solutions to the 3D Navier–Stokes equations with analytic forcing, arXiv:2609.20803: for a smooth, compactly supported vector field v : Vec3 → Vec3, the gradient energy ∫ ∑ᵢⱼ (∂ⱼvᵢ)² splits as ∫ ‖curl v‖² plus ∫ (div v)².

The proof expands both sides pointwise: ∑ᵢ (curl v)ᵢ² equals ∑ᵢⱼ (∂ⱼvᵢ)² - ∑ᵢⱼ ∂ⱼvᵢ ∂ᵢvⱼ, so the identity reduces to showing ∫ ∑ᵢⱼ ∂ⱼvᵢ ∂ᵢvⱼ = ∫ (∑ⱼ ∂ⱼvⱼ)². This cross-term identity is proved by two integrations by parts (moving ∂ⱼ off vᵢ and ∂ᵢ back onto vⱼ), with the symmetry of the second derivative used in between to commute the mixed partial ∂ⱼ∂ᵢvⱼ to ∂ᵢ∂ⱼvⱼ.

The curl of a time-independent vector field v : Vec3 → Vec3, with components (∂₂v₃ - ∂₃v₂, ∂₃v₁ - ∂₁v₃, ∂₁v₂ - ∂₂v₁).

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    Regularity helpers #

    The i-th component of a smooth vector field is smooth.

    The derivative of the i-th component of a smooth vector field in a fixed direction is again smooth.

    fderiv ℝ (v · i) · (basisVec j) is continuous for a smooth vector field.

    The second derivative ∂ₖ∂ⱼvᵢ is continuous for a smooth vector field.

    The second derivative ∂ₖ∂ⱼvᵢ has compact support.

    fderiv ℝ (v · i) · (basisVec j) is differentiable everywhere.

    A product of two continuous functions, one of them compactly supported, is integrable.

    theorem CIV.integral_sum_sum_eq (f : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 → ℝ) (hf : ∀ (i j : Fin 3), MeasureTheory.Integrable (f i j) MeasureTheory.volume) :
    ∫ (x : CKN.Foundation.Parabolic.Vec3), ∑ i : Fin 3, ∑ j : Fin 3, f i j x = ∑ i : Fin 3, ∑ j : Fin 3, ∫ (x : CKN.Foundation.Parabolic.Vec3), f i j x

    Pushing a finite double integral of a sum inside, or pulling it back out.

    Symmetry of the second derivative #

    Mixed partial derivatives of a smooth scalar function on Vec3 commute.

    The cross-term identity #

    For a compactly supported smooth vector field, ∫ ∂ⱼvᵢ ∂ᵢvⱼ = ∫ ∂ᵢvᵢ ∂ⱼvⱼ. This is the key cancellation lemma for the elliptic identity: two integrations by parts, moving ∂ⱼ off vᵢ and ∂ᵢ back onto vⱼ, with the symmetry of the second derivative used in between to commute ∂ⱼ∂ᵢvⱼ to ∂ᵢ∂ⱼvⱼ.

    The double-sum cross-term identity: ∫ ∑ᵢⱼ ∂ⱼvᵢ ∂ᵢvⱼ = ∫ (∑ⱼ ∂ⱼvⱼ)².

    The elliptic identity #

    The elliptic identity ‖∇v‖² = ‖curl v‖² + ‖div v‖² for a smooth compactly supported vector field on ℝ³.