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Tensor Q1 nodal interpolation has a first-order H1 error bound

Statement

Let d∈{2,3} and let the unit cube be partitioned into uniform tensor cells of side length h=1/N. Let g∈C1([0,1]d) have Lipschitz gradient with constant Mg, meaning ∣∇g(x)−∇g(y)∣≤Mg∣x−y∣ for all x,y. Let Ihg be the continuous tensor-product, degree-one nodal interpolant matching g at every grid vertex. Then Ihg lies in the tensor-product degree-one C0 spline space and ∥g−Ihg∥H1((0,1)d)≤CdhMg,Cd:=d+d+2d−1dd.

Facts & Assumptions

Given: The unit tensor grid, g and its Lipschitz-gradient constant, and the nodal interpolant described in the Statement.

[F1]

B-spline spaces and knot conventions defines degree-one tensor spline factors, and B-spline basis properties and polynomial reproduction gives their piecewise polynomial, continuity, partition and polynomial reproduction properties. On each cell, the tensor nodal shape functions are the products of the two endpoint linear factors in each coordinate; products of the one-dimensional partition/reproduction identities give ∑νϕν=1 and ∑ν(xν)rϕν=xr for each coordinate r. Hence they reproduce every affine function.

[F2]

For a C1 function with Mg-Lipschitz gradient, integration along the line segment from x0 to x gives ∣g(x)−g(x0)−∇g(x0)⋅(x−x0)∣≤12Mg∣x−x0∣2,∣∇g(x)−∇g(x0)∣≤Mg∣x−x0∣.

Proof

1.1F1F2given

Fix a cell K and one vertex x0. Put ℓ(x)=g(x0)+∇g(x0)⋅(x−x0) and r=g−ℓ. The cell diameter is d h, so [F2] gives ∣r(x)∣≤(d/2)h2Mg on K and ∣∇r(x)∣≤d hMg. The tensor Q1 interpolant reproduces ℓ, hence g−IKg=r−IKr.

2.1F1step 1.1algebra

Let ϕν be the 2d tensor nodal shape functions. They satisfy ϕν≥0, ∑νϕν=1, and ∣∇ϕν∣≤d/h. Thus ∣IKr∣≤(d/2)h2Mg and ∣∇IKr∣≤∑ν∣r(xν)∣∣∇ϕν∣≤2d−1dd hMg. Combining these with step 1.1 yields ∣g−IKg∣≤dh2Mg and ∣∇(g−IKg)∣≤(d+2d−1dd)hMg.

3.1F1step 2.1givenalgebra∎

Adjacent cells use the same vertex values, so their local interpolants agree on their common faces; consequently Ihg is continuous and belongs to the tensor degree-one spline space defined by [F1]. Square the pointwise bounds of step 2.1, integrate on each cell, and sum over the unit-volume partition. The resulting global L2 errors are at most dh2Mg and (d+2d−1dd)hMg for value and gradient. Since h≤1, the Euclidean combination defining the H1 norm is at most their sum, which is bounded by CdhMg.

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