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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: , , , , , admissible mean-zero data, and either stated pressure-correction algorithm.
In the backward-Euler algorithm the predictor matrix is ; in BDF2 it is . 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).
The periodic componentwise Laplacian and the seminorm satisfy by finite periodic reindexing (Periodic staggered-grid velocity and pressure spaces).
has zero mean and is bijective (Periodic pressure Laplacian gauge, solvability, and uniform Poincare bound).
A linear endomorphism of a finite-dimensional space with zero kernel is invertible by rank-nullity (Rank-nullity: ); is finite-dimensional because it is a finite face-array space.
Proof
For any nonzero , the componentwise Laplacian definition and finite periodic reindexing give Therefore . The predictor matrix has zero kernel and is invertible by [F4], so the backward-Euler predictor has a unique solution.
Similarly, . The BDF2 predictor matrix has zero kernel and is invertible by [F4], so its predictor is unique for either pressure-update branch.
For either predictor, summing 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 solving that equation.
The velocity and pressure updates are explicit after the unique predictor and pressure increment. Since , the corrected divergence is in backward Euler and in BDF2. The BDF2 rotational pressure correction subtracts , which has zero mean by compatibility; thus both pressure updates stay in .
Depends on
- Periodic staggered-grid velocity and pressure spaces
- Backward-Euler incremental pressure correction on a periodic staggered grid
- BDF2 standard and rotational incremental pressure-correction variants
- Periodic pressure Laplacian gauge, solvability, and uniform Poincare bound
- Rank-nullity: $\dim_F V=\operatorname{nullity}T+\operatorname{rank}T$
Used by
- One staggered Fourier mode is removed exactly by pressure correction Example
- First-order velocity accuracy for smooth periodic Stokes data Theorem
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
- J. L. Guermond, P. Minev, and J. Shen, An overview of projection methods for incompressible flows (standard reference, not scraped)