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LeanPool.ViscositySolutionTheory.ViscositySolns.Applications.Laplace.Weyl.PolarCoord

Integration in polar coordinates (ported from TauCeti) #

Let E be a nontrivial finite-dimensional real normed space of dimension n with an additive Haar measure μ. Mathlib's MeasureTheory.Measure.measurePreserving_homeomorphUnitSphereProd identifies μ on E \ {0} with the product of the surface measure μ.toSphere on the unit sphere and the radial measure r ^ (n - 1) dr on (0, ∞), but upstream only integrates radial functions against it (MeasureTheory.integral_fun_norm_addHaar). This file records the integral formula for an arbitrary integrable function, in both orders of integration,

∫ x, f x ∂μ = ∫ u ∈ S, ∫ r in (0, ∞), r ^ (n - 1) • f (r • u) ∂μ.toSphere = ∫ r in (0, ∞), r ^ (n - 1) • ∫ u ∈ S, f (r • u) ∂μ.toSphere.

Main declarations #

Provenance #

Pool port: imports relocated under LeanPool.ViscositySolutionTheory; original mathematical namespaces and copyright retained; checked with Lean/Mathlib v4.34.0.

Integration against MeasureTheory.Measure.volumeIoiPow k is integration on (0, ∞) against the weight r ^ k.

Integration in polar coordinates. An integrable function on a finite-dimensional real normed space is integrated by first integrating along each ray r ↦ r • u, against the radial Jacobian r ^ (d - 1), and then over the unit sphere against μ.toSphere.

Integration in polar coordinates, radial variable outermost. An integrable function on a finite-dimensional real normed space is integrated by first integrating over the sphere of radius r (parametrized by the unit sphere against μ.toSphere), and then in r against the radial Jacobian r ^ (d - 1).

The integral of f over the sphere of radius r about the origin, parametrized by the unit sphere, depends continuously on r ∈ [0, R] when f is continuous on the closed ball of radius R.