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Exact Newtonian coordinate flux on every centred sphere

Proved
HunterPDE.Newtonian.fundamentalSolution_sphere_flux

by Mazecto · Oct 10, 2026 · Mathlib 0df444a (Lean v4.33.1)

multivariable-calculusnewtonian-potentialpdesingular-integrals

Let n≥2n\ge2n≥2, R>0R>0R>0, and let Γ\GammaΓ be the Newtonian fundamental solution. For every coordinate pair i,ji,ji,j,

Rn−1∫Sn−1∂iΓ(−Rw)wj dS(w)=δijn.R^{n-1}\int_{S^{n-1}}\partial_i\Gamma(-Rw)w_j\,dS(w)=\frac{\delta_{ij}}n.Rn−1∫Sn−1​∂i​Γ(−Rw)wj​dS(w)=nδij​​.

The signed flux is independent of the radius. It supplies the spherical correction in the Hessian representation and the cancellation of the Hessian kernel over concentric annuli.

Preamble
import Theorems.Thm_MeasureTheory_integral_sphere_coordinate_mul
import Theorems.Thm_HunterPDE_Newtonian_fundamentalSolution_partial
import Mathlib.MeasureTheory.Measure.Haar.Unique
import Mathlib.Tactic.FieldSimp
import Mathlib.Tactic.Ring
open MeasureTheory HunterPDE.Newtonian
Formal statement
theorem HunterPDE.Newtonian.fundamentalSolution_sphere_flux (n : ℕ) (hn : 2 ≤ n) (R : ℝ) (hR : 0 < R) (i j : Fin n) :
    R ^ (n - 1) *
      (∫ (w : Metric.sphere (0 : EuclideanSpace ℝ (Fin n)) 1),
        partialDeriv (fundamentalSolution n) i (-(R • w.1)) * w.1 j ∂volume.toSphere) =
      1 / (n : ℝ) * (if i = j then 1 else 0) := by sorry
Source
Hunter, Notes on Partial Differential Equations, revised 6/18/2014, https://www.math.ucdavis.edu/~hunter/pdes/ch2.pdf, printed p. 39, Corollary 2.27 proof, the sphere flux calculation following equation (2.29).

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