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TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-24
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A solid between continuous graphs over a compact Jordan base is Jordan measurable and integrates by vertical sections

Statement

Let D⊆Rm be compact and Jordan measurable, let α,β:D→R be continuous with α≤β, and put K:={(u,t):u∈D,α(u)≤t≤β(u)}. The solid K is compact and Jordan measurable, and every continuous H:K→R satisfies ∫KH=∫D(∫α(u)β(u)H(u,t) dt)du.

Facts & Assumptions

Given: The data in the Statement, with integrals understood in the multidimensional Riemann sense.

[F2]

Every continuous real function on a compact Jordan measurable set is Riemann integrable (A continuous real function on a compact Jordan measurable set is Riemann integrable over that set).

[F3]

If E⊆Rp+q is bounded Jordan, g:E→R is integrable, and outside a content-zero parameter set the sections Ex are Jordan measurable and the restrictions gx are integrable, then the completed section-integral function is integrable and ∫Eg=∫(∫Exgx) dx; the symmetric coordinate order also holds (Fubini over a bounded Jordan set when all but a content-zero family of sections are integrable).

[F4]

Continuous real functions on a nonempty compact metric space attain finite extrema and are bounded (A continuous real-valued function on a nonempty compact metric space is bounded and attains a greatest and a least value).

Proof

technique · direct
1.1givenF4F5algebra

If D=∅, every assertion and both integrals are zero. Otherwise [F4] bounds α and β; the defining weak inequalities make K closed, so it is closed and bounded and therefore compact by [F5].

2.1step 1.1F1

By [F1] the boundary of the bounded set K has content zero, so the Jordan boundary criterion makes K Jordan measurable.

3.1step 2.1F2F3

By [F2], H is integrable on K. For each u∈D, the vertical section is exactly [α(u),β(u)], and the restriction t↦H(u,t) is continuous and integrable; [F3] therefore gives the displayed iterated formula.

4.1step 3.1algebra∎

If α(u)=β(u), the corresponding section is a singleton and its integral is zero. Thus coincident graphs, whether at isolated points or everywhere, require no exceptional convention.

Depends on

Used by

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Sources