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Well-definedness of the periodic pressure-correction solves

Statement

On the periodic staggered grid of Periodic staggered-grid velocity and pressure spaces, every admissible backward- Euler step of Backward-Euler incremental pressure correction on a periodic staggered grid and every admissible BDF2 step of BDF2 standard and rotational incremental pressure-correction variants has a unique predictor, a unique mean-zero pressure increment, and a unique updated pair. Both algorithms preserve the zero-mean pressure gauge and exact discrete incompressibility.

Facts & Assumptions

Given: d≥1, N≥2, h=1/N, ν>0, k>0, admissible mean-zero data, and either stated pressure-correction algorithm.

[F1]

In the backward-Euler algorithm the predictor matrix is I+kνAh; in BDF2 it is (3/(2k))I+νAh. The right-hand sides and pressure updates are exactly those in the two algorithm definitions (Backward-Euler incremental pressure correction on a periodic staggered grid, BDF2 standard and rotational incremental pressure-correction variants).

[F2]

The periodic componentwise Laplacian and the seminorm satisfy (Ahv,v)Mh=hd−2∑i,ℓ,j∣vi,j+eℓ−vi,j∣2≥0 by finite periodic reindexing (Periodic staggered-grid velocity and pressure spaces).

[F3]

Dhv has zero mean and Δh:Qh→Qh is bijective (Periodic pressure Laplacian gauge, solvability, and uniform Poincare bound).

[F4]

A linear endomorphism of a finite-dimensional space with zero kernel is invertible by rank-nullity (Rank-nullity: dim⁡FV=nullity⁡T+rank⁡T); Vh is finite-dimensional because it is a finite face-array space.

Proof

1.1givenF1F2F4algebra

For any nonzero v∈Vh, the componentwise Laplacian definition and finite periodic reindexing give (Ahv,v)Mh=hd−2∑i,ℓ,j∣vi,j+eℓ−vi,j∣2≥0. Therefore ((I+kνAh)v,v)Mh=∥v∥Mh2+kν(Ahv,v)Mh>0. The predictor matrix has zero kernel and is invertible by [F4], so the backward-Euler predictor has a unique solution.

2.1givenF1F2F4step 1.1algebra

Similarly, (((3/(2k))I+νAh)v,v)Mh=(3/(2k))∥v∥Mh2+ν(Ahv,v)Mh>0. The BDF2 predictor matrix has zero kernel and is invertible by [F4], so its predictor is unique for either pressure-update branch.

3.1F1F3step 1.1step 2.1

For either predictor, summing Dhu~ over all cells cancels the two occurrences of each periodic face value. Hence the right-hand side of the corresponding pressure-increment equation has zero mean. By [F3], there is exactly one mean-zero ϕn+1 solving that equation.

4.1F1F2F3step 3.1algebra∎

The velocity and pressure updates are explicit after the unique predictor and pressure increment. Since DhGh=Δh, the corrected divergence is Dhu~−kΔhϕ=0 in backward Euler and Dhu~−(2k/3)Δhϕ=0 in BDF2. The BDF2 rotational pressure correction subtracts νDhu~, which has zero mean by compatibility; thus both pressure updates stay in Qh.

Depends on

Used by

Cited to discharge well-definedness by Backward-Euler incremental pressure correction on a periodic staggered grid and BDF2 standard and rotational incremental pressure-correction variants.

Dependency tree · two levels

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Sources