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Weak Stokes solvability on bounded connected Lipschitz domains
Statement
Assume Countable Choice. Let be nonempty, bounded, connected and Lipschitz, or , and let . For every bounded linear functional on equipped with , there is a unique , , satisfying for every . The pressure is normalized to have mean zero. One stability bound is and .
Facts & Assumptions
Given: Countable Choice; a bounded connected Lipschitz ; the real Sobolev spaces; and .
Countable Choice is assumed by the Hilbert-space completeness and Lax–Milgram branch used below; no full Axiom of Choice is used by the local Korn or Poincare arguments. (The Axiom of Countable Choice ())
is Hilbert under Countable Choice, is its closed subspace, and bounded-domain Poincare makes the gradient norm equivalent to the H1 norm. (The Sobolev space is a Hilbert space, Zero-boundary Sobolev space as a norm closure, A bounded-domain Poincare inequality for H1-zero fields, The Axiom of Countable Choice ())
Real is Hilbert under Countable Choice, and the integral functional is bounded by , so its zero-mean kernel is closed and Hilbert. ( with the integral pairing is a Hilbert space, Holder's inequality for integrals, including the endpoint cases, The Axiom of Countable Choice ())
for every zero-boundary field. (The homogeneous Dirichlet strain identity)
The divergence form is bounded and has continuous inf-sup constant at least . (Continuous Stokes divergence inf-sup on a Lipschitz domain)
On real Hilbert spaces, bounded , coercivity on the constraint kernel and positive inf-sup imply unique mixed solvability with the stated norm bounds. (Babuska-Brezzi solvability by kernel coercivity and inf-sup)
Every zero-boundary velocity has zero-mean divergence. (Zero mean of the divergence of a zero-boundary field)
The L2 Cauchy--Schwarz inequality gives . (Cauchy-Schwarz inequality for )
Proof
By [F1], is complete in the H1 norm. If is Cauchy in , [F1] and Poincare make it Cauchy in H1; its H1 limit is in the closed subspace and its gradients converge. Thus is Hilbert in the gradient norm. By [F2], is Hilbert.
Cauchy–Schwarz and give . By [F3], on all of , hence on ; take and .
The form has and inf-sup by [F4]. Apply [F5] with . It yields a unique velocity and a unique mean-zero pressure satisfying the two displayed equations. The bound on velocity is .
By [F6], . The constraint equation tested with therefore gives , so the weak constraint is exact incompressibility. Also [F5] gives . Use , and the velocity estimate of step 3.1 to obtain . Mean-zero gauge is part of , so the pressure is unique in that normalization.
Depends on
- Stokes velocity and pressure spaces and weak forms
- A bounded-domain Poincare inequality for H1-zero fields
- The homogeneous Dirichlet strain identity
- Continuous Stokes divergence inf-sup on a Lipschitz domain
- Babuska-Brezzi solvability by kernel coercivity and inf-sup
- The Sobolev space $H^1$ is a Hilbert space
- The Axiom of Countable Choice ($\mathrm{AC}_\omega$)
- Holder's inequality for integrals, including the endpoint cases
- $L^2$ with the integral pairing is a Hilbert space
- Zero mean of the divergence of a zero-boundary field
- Zero-boundary Sobolev space as a norm closure
- Cauchy-Schwarz inequality for $L^2$
Used by
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Sources
- Jean-Luc Guermond, MATH 661 Fall 2025, Chapters 49–54 (complete course notes) (standard reference, not scraped)
- Daniele Boffi, Franco Brezzi, Michel Fortin, Mixed Finite Element Methods and Applications (complete textbook) (standard reference, not scraped)