The divergence theorem on a manifold without boundary #
On a smooth manifold without boundary with a C¹ Riemannian metric, the divergence of a
compactly supported C¹ vector field has integral zero against the Riemannian volume:
∫ div X dV = 0.
Integrating the product rule div (f X) = f div X + df(X) then gives the integration-by-parts
formulas for the divergence and the Laplace–Beltrami operator Δ = div ∘ grad:
∫ f div X dV = -∫ df(X) dV, ∫ f Δg dV = -∫ ⟪grad f, grad g⟫ dV, ∫ f Δg dV = ∫ (Δf) g dV.
These identities underlie the energy (weak) formulation of second-order operators on closed
manifolds. No orientation is used: the measure is the orientation-free TauCeti.riemannianVolume.
Main results #
TauCeti.Manifold.integral_divergence_eq_zero: the divergence theorem∫ div X dV = 0.TauCeti.Manifold.integral_laplaceBeltrami_eq_zero:∫ Δf dV = 0for a compactly supportedC²functionf.TauCeti.Manifold.integral_mul_divergence,TauCeti.Manifold.integral_mul_divergence_of_hasCompactSupport_right:∫ f div X dV = -∫ df(X) dVwhenforXhas compact support.TauCeti.Manifold.integral_mul_laplaceBeltrami: Green's first identity∫ f Δg dV = -∫ ⟪grad f, grad g⟫ dV.TauCeti.Manifold.integral_mul_laplaceBeltrami_right_eq_left: Green's second identity∫ f Δg dV = ∫ (Δf) g dV.TauCeti.Manifold.integrable_divergence: the divergence of a compactly supportedC¹field is integrable.
Implementation notes #
The proof is chart by chart. In the chart at α, with chart frame e₁, …, eₙ, volume density ρ
and frame coefficients Xᵏ, the coordinate formula ρ div X = ∑ₖ ∂ₖ (ρ Xᵏ)
(TauCeti.chartVolumeDensity_mul_divergence) turns the integral of the divergence of a field
supported in the chart into a sum of integrals of partial derivatives of compactly supported C¹
functions on the model space, each of which vanishes. A smooth partition of unity subordinate to
the chart sources reduces a general compactly supported field to finitely many such fields; this
is where the manifold is assumed smooth, while the metric need only be C¹.
References #
- J. M. Lee, Introduction to Smooth Manifolds, 2nd ed., Springer GTM 218 (2013), Chapter 16 (the divergence theorem, Theorem 16.32, and Green's identities).
- J. M. Lee, Introduction to Riemannian Manifolds, 2nd ed., Springer GTM 176 (2018), Chapter 2 (the divergence and the Riemannian density).
The divergence of a compactly supported C¹ vector field is integrable against the Riemannian
volume.
The divergence theorem on a manifold without boundary: the divergence of a compactly
supported C¹ vector field has integral zero against the Riemannian volume.
Integration by parts for the divergence: for a compactly supported C¹ function f and a
C¹ vector field X on a manifold without boundary, ∫ f div X dV = -∫ df(X) dV.
Integration by parts for the divergence, for a compactly supported field: for a C¹
function f and a compactly supported C¹ vector field X on a manifold without boundary,
∫ f div X dV = -∫ df(X) dV.
The Laplace--Beltrami operator of a compactly supported C² function on a manifold
without boundary has integral zero against the Riemannian volume.
Green's first identity on a manifold without boundary: for a compactly supported C¹
function f and a C² function g, ∫ f Δg dV = -∫ ⟪grad f, grad g⟫ dV.
The energy identity for a compactly supported C² eigenfunction of the scalar Laplacian
on a manifold without boundary, using the convention Δf = -λ f.
Green's second identity on a manifold without boundary: for a compactly supported C²
function f and a C² function g, ∫ f Δg dV = ∫ (Δf) g dV.