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Reynolds transport identity on an ALE moving domain

Statement

Assume Countable Choice and d≥2. Let At be the ALE moving-domain map of ALE moving-domain map and mesh velocity, and let g(x,t) and its first derivatives be continuous on the moving closure. Then, for each t∈(0,T),

ddt∫Ω(t)g(x,t) dx=∫Ω(t)∂tg(x,t) dx+∫∂Ω(t)g(x,t)wm(x,t)⋅n(x,t) dS.

Here n is the outward normal from the transported finite piecewise-C1 boundary presentation. This is a continuous transport identity; no discrete high-dimensional geometric conservation estimate follows from it.

Facts & Assumptions

Given: Assume Countable Choice, an ALE moving-domain map At, its Jacobian J, its mesh velocity wm, and a scalar field g with the stated space-time regularity.

[A1]

The Axiom of Countable Choice (ACω): Countable Choice, written ACω, is the axiom that every countable family of nonempty sets has a choice function.

[F1]

ALE moving-domain map and mesh velocity: At is a C2 orientation-preserving diffeomorphism, J=det⁡DξAt>0, and wm(At(ξ),t)=∂tAt(ξ).

[F2]

Jacobi identity for the ALE mesh Jacobian: ∂tJ=J div⁡xwm.

[F3]

Specified finite piecewise C1 boundary presentations: the boundary has a specified finite set of compact C1 faces and a compact edge set, with overlaps and edges surface-null and an outward normal on each face off the edges.

[F4]

Change of variables for an injective C1 map on a compact Jordan set: an injective C1 map with invertible derivative sends a compact Jordan set to a compact Jordan set; for a bounded integrand, the change-of-variables formula applies when the image integrand (equivalently its pullback) is Riemann integrable.

[F5]

Divergence for finite piecewise C1 presentations: under ACω, a C1 vector field on a specified finite piecewise-C1 domain satisfies ∫Ωdiv⁡F=∫∂ΩF⋅n dS.

[F6]

The mean value theorem, as the case g(x)=x of Cauchy's: for f continuous on [a,b] with a<b and differentiable on (a,b) there is c∈(a,b) with f(b)−f(a)=f′(c)(b−a): a scalar function continuous on a closed interval and differentiable in its interior has a point where its derivative equals the interval's average rate of change.

[F7]

The Riemann integral of a bounded function over a bounded Jordan measurable set and Linearity, monotonicity, the absolute-value estimate and coordinate-slice additivity for the Riemann integral in Rm: Jordan integrals are integrals of zero extensions on bounding rectangles, where linearity, monotonicity, and the absolute-value estimate hold.

[F8]

A bounded set is Jordan measurable iff its indicator is Riemann integrable, and the integral is its Jordan content: the integral of the indicator of a compact Jordan set is its finite Jordan content.

[F9]

Heine-Cantor: a continuous map from a compact metric space to any metric space is uniformly continuous: a continuous function on a compact metric space is uniformly continuous.

[F10]

A continuous real function on a compact Jordan measurable set is Riemann integrable over that set: every continuous real function on a compact Jordan set is Riemann integrable there.

[F11]

A bounded set in Rm is Jordan measurable iff its boundary is null, equivalently of content zero: a bounded set is Jordan measurable exactly when its boundary is null, equivalently has Jordan content zero.

[F12]

Lebesgue's criterion in Rm: a bounded function on a closed nondegenerate rectangle is Riemann integrable iff its discontinuity set is null: a bounded function on a closed bounding rectangle whose discontinuities lie in a null set is Riemann integrable.

[F13]

Borel Darboux integrands in finite dimension: under ACω, a bounded Borel Riemann-integrable function on a nondegenerate closed box is Lebesgue integrable with the same integral. The volume integral in [F5] uses Lebesgue measure.

Proof

1.1F1F4F11construct

Put K^=Ω^‾, Kt=At(K^)=Ω(t)‾, and let Bt=∂Ω(t) and B^=∂Ω^. Cover each compact face in either finite boundary presentation by finitely many smaller regular C1 graph charts with bounded base and bounded graph derivative. For a base grid of side δ, each chart needs at most Cδ−(d−1) base cubes; the Lipschitz bound places each graph portion in an axis-parallel d-cube of side C′δ. The total covering volume is at most C′′δ, which tends to zero. Since there are finitely many faces, both boundaries are compact Jordan sets of content zero. By [F11] they are null and the open domains are Jordan measurable; by the compact-image conclusion in [F4], Kt is compact Jordan.

2.1F4F7F8F10F12step 1.1algebra

For any continuous h on Kt, its zero extensions from Ω(t) and Kt to a nondegenerate closed rectangle containing Kt in its interior are bounded and have discontinuities only on Bt, a null set, so [F12] makes them integrable. Their difference is supported on Bt and bounded in absolute value by a constant times 1Bt. By [F8], ∫1Bt=0, and [F7] shows the two integrals agree. The same argument applies to K^ and Ω^. By [F10], continuous integrands on the compact closures are integrable, so [F4] applies to the compact closures. Consequently, for G(ξ,t):=g(At(ξ),t)J(ξ,t), I(t):=∫Ω(t)g dx=∫K^G(ξ,t) dξ=∫Ω^G(ξ,t) dξ.

3.1F6F7F8F9F10step 2.1algebra

For small nonzero h, apply [F6] to s↦G(ξ,s) between t and t+h. The difference quotient equals ∂tG(ξ,θξ) at an intermediate time. By [F9], ∂tG is uniformly continuous on K^ times a compact time neighborhood of t, so these quotients converge uniformly in ξ to ∂tG(ξ,t). The derivative and difference quotients are continuous on the compact Jordan set K^, hence integrable by [F10]. [F7] and [F8] bound the integral of their difference by its uniform norm times cont⁡(K^). Since I(t)=∫K^G(ξ,t) dξ by step 2.1, I′(t)=∫K^∂tG(ξ,t) dξ. The chain and product rules then give I′(t)=∫K^J(∂tg+∇xg⋅wm)+g∂tJ dξ.

4.1F2F4F10step 2.1step 3.1algebra

Substitute [F2] into step 3.1 and use ∇xg⋅wm+gdiv⁡xwm=div⁡x(gwm). The resulting integrand is continuous on the moving closure. Apply [F4] to the compact closures and use the open/closed integral equality from step 2.1 to obtain I′(t)=∫Ω(t)(∂tg+div⁡x(gwm)) dx.

5.1A1F3F5F13step 2.1step 4.1∎

Set f=div⁡x(gwm) and choose a nondegenerate closed box Q containing Kt in its interior. The field gwm is C1 on the moving closure, so f is continuous and bounded there. Its zero extension f~ from the open set Ω(t) to Q is Borel: each strict superlevel is a relatively open subset of Ω(t), together with Q∖Ω(t) when the level is negative. Step 2.1 gives its Riemann integrability. By [A1] and [F13], its Riemann integral over Q equals its Lebesgue integral, which is the Lebesgue integral of f over Ω(t). Thus the Jordan volume integral in step 4.1 is exactly the volume integral used by [F5]. Apply [F5] to gwm on the finite piecewise-C1 presentation [F3] to obtain ∫Ω(t)div⁡x(gwm) dx=∫∂Ω(t)gwm⋅n dS. Substitution into step 4.1 proves the asserted identity. Countable Choice is used through [F5] and [F13].

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