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An exact one-form has zero period on every closed piecewise-C¹ curve

Statement

On any smooth manifold M, if a smooth one-form ω is exact, so ω=dϕ for a globally defined smooth scalar ϕ:M→R, then Per⁡γ(ω)=0 for every closed piecewise-C1 curve γ in M.

Facts & Assumptions

Given: A smooth exact one-form ω=dϕ on a smooth manifold M and a closed piecewise-C1 curve γ:[0,1]→M with an admissible finite subdivision.

[F1]

Period of a smooth one-form along a closed curve: on a smooth manifold, for a smooth one-form and a closed continuous piecewise-C1 curve with finitely many chartwise pieces and one-sided endpoint derivatives, the period is the sum of the integrals of ωγ(t)(γ˙(t)) over those pieces.

[F2]

Closed and exact differential forms: exactness means ω=dϕ for a globally defined smooth scalar ϕ.

[F3]

The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a): in local coordinates, the total derivative of a composition is the composition of the total derivatives.

[F4]

A continuous function on [a,b] is Riemann integrable, by Heine-Cantor and Riemann's criterion: each continuous derivative on a closed subinterval is integrable there.

[F5]

The second fundamental theorem: if G is differentiable on [a,b] with G′=f and f is integrable, then ∫abf=G(b)−G(a): if h is differentiable on a closed interval and h′ is integrable, then the integral of h′ equals the endpoint increment of h.

Proof

1.1givenF1F2F3F4algebra

Fix the finite subdivision from [F1]. On each chartwise C1 piece choose a chart κ:U→V⊆Rn containing its image, and put x(t):=κ(γ(t)) and ϕ~:=ϕ∘κ−1. By [F2] the coordinate coefficients of ω are ∂iϕ~; applying [F3] to ϕ~∘x gives ddt(ϕ∘γ)(t)=ωγ(t)(γ˙(t)) in the piece interior. The same formula holds with one-sided derivatives at the endpoints: the differentiability expansion of ϕ~ composed with the one-sided expansion of x gives Dϕ~(x(t))x′(t). These derivatives are continuous on the closed piece by [F1] and smoothness of ϕ, so they are integrable by [F4].

2.1givenF1F5step 1.1algebra∎

Apply [F5] on each subdivision interval to h=ϕ∘γ. By [F1] the period is the sum of those integrals, so it equals the sum of the increments ϕ(γ(tj+1))−ϕ(γ(tj)). The internal endpoint terms cancel, and the remaining increment is ϕ(γ(1))−ϕ(γ(0))=0 because γ is closed. Thus the period is zero.

Depends on

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