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Babuska-Brezzi solvability by kernel coercivity and inf-sup

Statement

Assume Countable Choice. Let V,Q be real Hilbert spaces, and let a:V×V→R and b:V×Q→R be bounded bilinear forms. If Q={0}, the theorem reduces to Lax–Milgram on V with Z=V and p=0. Otherwise, if Q≠{0}, assume V≠{0}. Define B:V→Q by (Bv,q)Q=b(v,q) and set β:=inf⁡q≠0sup⁡v≠0b(v,q)/(∥v∥V∥q∥Q)>0. Suppose Z:=ker⁡B is closed and a(z,z)≥α∥z∥V2 on Z, with α>0. For every F∈V′ and G∈Q′, there is a unique (u,p)∈V×Q satisfying a(u,v)+b(v,p)=F(v),b(u,q)=G(q), for all v∈V,q∈Q. If Ma=∥a∥, then one stability bound is ∥u∥V≤β−1∥G∥+α−1(∥F∥+Maβ−1∥G∥),∥p∥Q≤β−1(∥F∥+Ma∥u∥V).

Facts & Assumptions

Given: Countable Choice, real Hilbert spaces, bounded a,b, β>0, and coercivity of a on Z.

[A1]

Countable Choice is required by the Lax–Milgram step on the closed constraint kernel. (The Axiom of Countable Choice (ACω))

[F1]

The inf-sup bound yields a bounded linear right inverse R:Q→V with BR=I and ∥R∥≤β−1. (Hilbert inf-sup gives a bounded constraint right inverse)

[F2]

Lax–Milgram gives a unique solution on the Hilbert subspace Z for a bounded coercive form, and its norm is controlled by the right-hand side divided by α. (The Lax--Milgram theorem, The Axiom of Countable Choice (ACω))

[F3]

Riesz representation identifies bounded functionals on V and Q with inner products against unique vectors. (Riesz representation for Hilbert spaces)

Proof

1.1A1F1F3

If Q={0}, then G=0, Z=V, and Lax–Milgram on V gives the unique solution (u,0) with ∥u∥≤α−1∥F∥; so suppose Q≠{0}. By [F3], write G(q)=(g,q)Q for a unique g∈Q with ∥g∥=∥G∥. Let ug=Rg using [F1]. Then Bug=g, ∥ug∥≤β−1∥G∥, and the constraint equation will hold for u=ug+z with any z∈Z.

2.1A1F2step 1.1

On the closed Hilbert subspace Z, solve a(z,w)=F(w)−a(ug,w) for all w∈Z by [F2]. The restricted form is bounded and coercive by hypothesis, and the functional norm is at most ∥F∥+Ma∥ug∥. Therefore ∥z∥≤α−1(∥F∥+Maβ−1∥G∥) and u=ug+z has the stated bound. The equation a(u,w)=F(w) holds for every w∈Z.

3.1A1F1givenstep 1.1step 2.1

Define ℓ(v)=F(v)−a(u,v). It vanishes on Z by step 2.1. Set Λ(q)=ℓ(Rq). This is bounded by ∥R∥∥ℓ∥∥q∥, and for every v, v−RBv∈Z, so ℓ(v)=ℓ(RBv)=Λ(Bv).

4.1A1F1F3step 3.1step 1.1

By [F3], there is a unique p∈Q with Λ(q)=(q,p)Q. Hence ℓ(v)=(Bv,p)Q=b(v,p), giving the first mixed equation; step 1.1 gives the second. Also ∥p∥≤β−1∥ℓ∥≤β−1(∥F∥+Ma∥u∥).

5.1A1F1givenF3∎

For uniqueness, subtract two solutions. Their velocity difference w lies in Z; testing the first difference equation with w gives a(w,w)=0, so coercivity gives w=0. The pressure difference then pairs to zero with every Bv; since [F1] makes B onto, it pairs to zero with all Q, hence is zero.

Depends on

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