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Yukawa shell theorem, interior potential

Proved
YukawaPotential.yukawaShellPotential_interior

by Lucas · Oct 3, 2026 · Mathlib 0df444a (Lean v4.33.1)

mathematical-physicsyukawa-potential

Let G,g∈RG,g\in\mathbb RG,g∈R, α>0\alpha>0α>0, m>0m>0m>0, and let VshellV^{\mathrm{shell}}Vshell be the potential of a uniform thin spherical shell of radius RRR and total scaling constant GGG centred at the origin, felt by a point of scaling constant ggg (see the definition item). For every x∈R3x\in\mathbb R^3x∈R3 with 0<∣x∣<R0<|x|<R0<∣x∣<R,

Vshell(x)=G g e−αmRR⋅sinh⁡(αm∣x∣)αm∣x∣.V^{\mathrm{shell}}(x) = G\,g\,\frac{e^{-\alpha m R}}{R}\cdot\frac{\sinh(\alpha m |x|)}{\alpha m |x|}.Vshell(x)=GgRe−αmR​⋅αm∣x∣sinh(αm∣x∣)​.

Unlike the Newtonian case, the interior potential is not constant.

Formalization Note The centre x=0x=0x=0 is excluded because the article's formula is there only defined as a limit (sinh⁡(αmr)/(αmr)→1\sinh(\alpha m r)/(\alpha m r)\to1sinh(αmr)/(αmr)→1), while Lean would evaluate sinh⁡(0)/0\sinh(0)/0sinh(0)/0 to 000. The hypotheses force R>0R>0R>0.

Preamble
import Mathlib
import Definitions.Def_YukawaPotential_Defs

open MeasureTheory Filter Topology
Formal statement
namespace YukawaPotential
theorem yukawaShellPotential_interior (G g α m R : ℝ) (hα : 0 < α) (hm : 0 < m)
    (x : EuclideanSpace ℝ (Fin 3)) (hx0 : 0 < ‖x‖) (hx : ‖x‖ < R) :
    yukawaShellPotential G g α m R x =
      G * g * (Real.exp (-(α * m * R)) / R) * (Real.sinh (α * m * ‖x‖) / (α * m * ‖x‖)) := by sorry
end YukawaPotential
Source
Wikipedia, "Yukawa potential", revision oldid=1371658231, https://en.wikipedia.org/w/index.php?title=Yukawa_potential&oldid=1371658231, section 'Spherical shell': the interior potential is V(r < R) = G g (e^{-αmR}/R) (sinh αmr)/(αmr).
Read-back

What the Lean code literally says, in plain math · Aristotle (Harmonic) — non-blind, same agent as the drafter

Non-blind read-back — not independent testimony. This read-back was written by the same agent (Aristotle, by Harmonic) that drafted the Lean statement it describes, with full knowledge of the source article and of the intended meaning. It was produced at the explicit request of the proposal owner and must not be mistaken for a blind, independent audit.

Fix real numbers G,gG,gG,g (arbitrary), real numbers α>0\alpha>0α>0, m>0m>0m>0, a real number RRR, and a point x∈R3x\in\mathbb R^3x∈R3 with 0<∣x∣<R0<|x|<R0<∣x∣<R (so R>0R>0R>0). Let

S(x)=G g 1σ(S2)∫S2e−αm∣x−Ru∣∣x−Ru∣ dσ(u),S(x) = G\,g\,\frac{1}{\sigma(S^2)}\int_{S^2}\frac{e^{-\alpha m|x-Ru|}}{|x-Ru|}\,d\sigma(u),S(x)=Ggσ(S2)1​∫S2​∣x−Ru∣e−αm∣x−Ru∣​dσ(u),

with S2S^2S2 the unit sphere in R3\mathbb R^3R3 and σ\sigmaσ its rotation-invariant surface measure from the cone construction (total mass 4π4\pi4π); the integral is a Bochner integral (defaulting to 000 if not integrable). The statement asserts

S(x)=G g⋅e−αmRR⋅sinh⁡(αm∣x∣)αm∣x∣.S(x) = G\,g\cdot\frac{e^{-\alpha m R}}{R}\cdot\frac{\sinh(\alpha m|x|)}{\alpha m|x|}.S(x)=Gg⋅Re−αmR​⋅αm∣x∣sinh(αm∣x∣)​.

The centre x=0x=0x=0 and the points with ∣x∣≥R|x|\ge R∣x∣≥R are not covered.

Human review
  • Endorsed by Shuze Chen · Oct 8, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 8, 2026

    Confirmed by the mission captain (proposal self-audit).

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