The Leibniz rule for the spatial Laplacian, in weak form #
The paper's identity eq:leibniz-lap,
Δ(η T) = η Δ T + 2 ∂_j η ∂_j T + T Δ η,
is stated there for a scalar distribution T and a smooth η. This file
proves the underlying pointwise second-order product rule for smooth functions
on Vec3 := Fin 3 → ℝ, and then integrates it against a locally integrable
weight to obtain the weak (test-function) form used in the paper.
Spatial partial derivatives are ordinary partial derivatives, expressed as the
Fréchet derivative applied to a coordinate basis vector, matching the
convention of CKN.spatialPartial.
Spatial partial derivatives and their product rules #
The ith spatial partial derivative ∂_i f, as the Fréchet derivative applied
to the ith coordinate basis vector.
Equations
- CKN.spatialDeriv f i x = (fderiv ℝ f x) (CKN.basisVec i)
Instances For
The spatial Laplacian Δ f = ∑_i ∂_i ∂_i f.
Equations
- CKN.spatialLaplacian f x = ∑ i : Fin 3, CKN.spatialDeriv (CKN.spatialDeriv f i) i x
Instances For
The Euclidean gradient pairing ∇f · ∇g = ∑_i ∂_i f ∂_i g.
Equations
- CKN.spatialGradDot f g x = ∑ i : Fin 3, CKN.spatialDeriv f i x * CKN.spatialDeriv g i x
Instances For
The mixed second derivative ∂_i ∂_j f.
Equations
- CKN.mixedSecond f i j x = CKN.spatialDeriv (CKN.spatialDeriv f j) i x
Instances For
The pointwise second-order product rule ∂_i ∂_j (η φ) of eq:leibniz-lap
and eq:commute.
The pointwise Leibniz rule eq:leibniz-lap for the spatial Laplacian:
Δ(η φ) = η Δφ + 2 ∇η · ∇φ + φ Δη.