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Exact space-time weak identity for the hydrostatic update

Statement

Let d,τ>0, Ii=[id,(i+1)d), tn=nτ, and Jn=[tn,tn+1). Suppose vector states and shared face fluxes satisfy d(Uin+1−Uin)+τ(F^i+1/2n−F^i−1/2n)=dτSin as in Hydrostatic reconstruction with a dry-safe HLL flux and one-sided pressure corrections. For φ∈Cc∞(R×(−∞,T);R2) define the space-time cell average Φin=1dτ∫Jn∫Iiφ(x,t) dx dt. Choose N such that φ vanishes for t≥tN−1. Then ∑id Ui0⋅Φi0+∑n=1N−1∑id Uin⋅(Φin−Φin−1)+∑n=0N−1∑iτ F^i+1/2n⋅(Φi+1n−Φin)+∑n=0N−1∑idτ Sin⋅Φin=0. Every sum is finite because the test is compactly supported.

Facts & Assumptions

Given: The vector finite-volume recurrence with shared face fluxes and cell source, the half-open space-time grid, and the cell-average test values above.

[F1]

Hydrostatic reconstruction with a dry-safe HLL flux and one-sided pressure corrections: the update is equivalent to d(Uin+1−Uin)+τ(F^i+1/2n−F^i−1/2n)=dτSin with one shared HLL flux at every face.

Proof

1.1F1given

Multiply the recurrence in [F1] by Φin using the Euclidean dot product and sum over cells i and time levels 0≤n<N. Compact support leaves only finitely many nonzero terms, and the resulting exact sum is zero.

2.1step 1.1algebra

For each cell, summing in time and using ΦiN−1=0 gives ∑n=0N−1(Uin+1−Uin)⋅Φin=−Ui0⋅Φi0+∑n=1N−1Uin⋅(Φin−1−Φin). This is finite summation by parts; no limit or infinite rearrangement is used.

3.1F1step 1.1step 2.1algebra∎

Reindexing the spatial face sum gives ∑i(F^i+1/2n−F^i−1/2n)⋅Φin=∑iF^i+1/2n⋅(Φin−Φi+1n). Insert this and step 2.1 into step 1.1, retain the source sum with its minus sign from [F1], and multiply the zero identity by −1. The displayed identity follows.

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