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Nodal feasibility can miss a nonconvex obstacle between vertices

Statement

Let Ω=(0,1)2, ΓD={0}×[1/4,3/4], ΓC={1}×[1/4,3/4], and n=(1,0). Use the grid x∈{0,1/2,1}, y∈{0,1/4,3/4,1} and split each rectangular cell by a diagonal. This is a matching triangular mesh on which both segments are single boundary edges. Parameterize ΓC by normalized arclength s=2(y−1/4)∈[0,1], set ψ(s)=−1+4s(1−s), and let vh(x,y)=(−x,0). The obstacle is continuous, nonpositive and concave, and vh satisfies both endpoint nodal inequalities, but vh∉K because its contact gap is negative at the midpoint.

Facts & Assumptions

Given: The nodal scheme Conforming nodal P1 Signorini contact discretization except that its convexity hypothesis on ψ is removed for this counterexample.

[F1]

The nodal constraints require vh(a)⋅n≥Ihψ(a) at each contact vertex; the continuum feasible set requires TCvh⋅n≥ψ almost everywhere on the whole contact segment. (Conforming nodal P1 Signorini contact discretization, The vector Signorini contact set and variational inequality)

[F2]

A real function is concave on an interval when its negative is convex there, with convexity defined by the chord inequality. (Convex, strictly convex, concave, strictly concave, and midpoint-convex real functions on an interval)

Proof

1.1F1F2givenalgebra

The polynomial ψ(s)=−1+4s(1−s) has endpoint values −1 and midpoint value 0, and ψ(s)=−(2s−1)2 shows its maximum is 0. For s0,s1∈[0,1] and t∈[0,1], direct expansion gives ψ((1−t)s0+ts1)−[(1−t)ψ(s0)+tψ(s1)]=4t(1−t)(s1−s0)2≥0, with strict inequality when 0<t<1 and s0≠s1. Thus [F2] says ψ is strictly concave, not convex, and the convex-obstacle premise is absent.

2.1F1givenalgebra∎

The vector field vh(x,y)=(−x,0) is affine on each triangle and is zero on ΓD, hence belongs to Vh. On the two contact vertices its normal value is −1, equal to the endpoint obstacle values, so both nodal inequalities hold. Along all of ΓC, vh⋅n=−1, while at s=1/2 the obstacle equals 0; continuity gives an interval around that midpoint on which −1<ψ(s). Therefore the continuum contact inequality fails on a set of positive arclength and vh∉K.

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