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A two-scale VMS closure attains its Schur defect bound

Example

Let each resolved and unresolved space be R with the absolute-value norm (and give its dual the corresponding dual norm). Take the block matrix (2112), load (1,0), and closure inverse T=1/4. The exact and modeled coarse solutions differ by exactly the defect bound in Finite-dimensional VMS residual closure has an explicit Schur defect bound.

Facts & Assumptions

Given: The two-block VMS decomposition and approximate closure, with scalar block entries Acc=Aff=2, Acf=Afc=1, load Fc=1, Ff=0, and T=1/4.

[F1]

Finite-dimensional resolved–unresolved VMS split and residual closure: if G=Aff−1, the exact coarse Schur system is (Acc−AcfGAfc)uc=Fc−AcfGFf and the modeled system replaces G by T.

[F2]

Finite-dimensional VMS residual closure has an explicit Schur defect bound: the coarse error is bounded by ∥S~−1∥∥Acf∥∥T−G∥∣Ff−Afcuc∣.

Verification

1.1F1givenalgebra

Here G=1/2, so the exact Schur coefficient is 2−1/2=3/2 and the exact coarse solution is uc=2/3. The exact unresolved component is uf=G(Ff−Afcuc)=−1/3.

2.1F1step 1.1algebra

Replacing G by T=1/4 gives the approximate Schur coefficient 2−1/4=7/4, hence u~c=4/7, and u~f=T(Ff−Afcu~c)=−1/7. The coarse error is ∣4/7−2/3∣=2/21.

3.1F1F2step 1.1step 2.1algebra∎

The bound in [F2] equals (4/7)⋅1⋅(1/4)⋅(2/3)=2/21, because ∥S~−1∥=4/7, ∣Acf∣=1, ∣T−G∣=1/4, and ∣Ff−Afcuc∣=2/3. Thus the defect bound is attained exactly in this finite example.

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