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Discrete weak identity for a conservative finite-volume update

Statement

Let (Ujm,n) be a scheme from Conservative two-point finite-volume schemes for scalar laws, with reconstruction (Um,Qm) as in Piecewise-constant finite-volume state and face-flux reconstructions. For a test function φ∈Cc∞(R×(−∞,T)), define its space-time cell average Φjm,n=1hmτm∫tnmtn+1m∫Ijmφ(x,t) dx dt. If N≥1 is such that φ vanishes for t≥tN−1m, then ∑j∈ZhmUjm,0Φjm,0+∑n=1N−1∑j∈ZhmUjm,n(Φjm,n−Φjm,n−1)+∑n=0N−1∑j∈ZτmQj+1/2m,n(Φj+1m,n−Φjm,n)=0. All sums are finite because φ is compactly supported in space and time.

Facts & Assumptions

Given: The grid, fluxes and update in Conservative two-point finite-volume schemes for scalar laws, the reconstruction convention in Piecewise-constant finite-volume state and face-flux reconstructions, and the test and terminal index in the Statement.

[F1]

The cell update is hm(Ujm,n+1−Ujm,n)+τm(Qj+1/2m,n−Qj−1/2m,n)=0. (Conservative two-point finite-volume schemes for scalar laws)

[F2]

The test averages Φjm,n are constant on each cell-time slab, and Qm=Qj+1/2m,n on Ijm×Jnm. (Piecewise-constant finite-volume state and face-flux reconstructions)

Proof

1.1F1F2given

Multiply [F1] by Φjm,n and sum over j∈Z and n=0,…,N−1. Only finitely many terms are nonzero, so the summed update is an exact finite sum equal to zero.

2.1step 1.1algebra

For each fixed j, telescoping gives ∑n=0N−1(Ujm,n+1−Ujm,n)Φjm,n=−Ujm,0Φjm,0+∑n=1N−1Ujm,n(Φjm,n−1−Φjm,n), since Φjm,N−1=0 by the terminal support condition.

3.1step 1.1step 2.1algebra∎

Reindex the spatial flux sum: ∑j(Qj+1/2m,n−Qj−1/2m,n)Φjm,n=∑jQj+1/2m,n(Φjm,n−Φj+1m,n). Substitute this and step 2.1 into step 1.1, then multiply the zero identity by −1 to obtain exactly the displayed formula.

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