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Boundary elimination returns exactly the finite Chebyshev collocation system

Statement

For the algorithm Boundary-eliminated Chebyshev collocation for a two-point Dirichlet BVP, a success output is the unique nodal vector with U0=g+, UN=g− satisfying

−(DN(2)U)i+a(xi)(DNU)i+b(xi)Ui=f(xi),1≤i<N,

where DN is the exact Chebyshev–Gauss–Lobatto differentiation matrix and DN(2)=DNDN. If the interior matrix is singular, the algorithm returns singular-interior-matrix and makes no claim about existence or uniqueness for the given right-hand side.

Facts & Assumptions

Given: An integer N≥2, node values of a,b,f, endpoints g−,g+, the boundary-elimination algorithm, and its interior matrix A.

[F1]

Boundary-eliminated Chebyshev collocation for a two-point Dirichlet BVP: Cij=−(DN2)ij+a(xi)(DN)ij+b(xi)δij, A=(Cij)1≤i,j<N, and ri=f(xi)−Ci0g+−CiNg−.

[F2]

Chebyshev–Gauss–Lobatto differentiation is exact on the interpolant: for the interpolant p through the full nodal vector U, DNU=(p′(xi))i; applying DN again gives (p′′(xi))i.

[F3]

Proof

1.1givenF1

On a success branch the algorithm sets U0=g+ and UN=g− and solves AUI=r for the interior vector UI=(U1,…,UN−1).

1.2givenF2

By [F2], DNU and DN(2)U are respectively the first and second derivatives of the degree-at-most-N nodal interpolant evaluated at the nodes.

2.1givenF1step 1.1step 1.2algebra

Expanding the ith row of the full expression using [F1] gives ∑j=1N−1CijUj+Ci0g++CiNg−=f(xi), which is exactly the reduced equation AUI=r with the definition of ri. Combined with step 1.2, this is the stated collocation equation at every interior node.

2.2givenF1F3step 1.1algebra

Since the success branch has invertible A, [F3] gives exactly one interior vector solving AUI=r. The prescribed endpoint values then give exactly one full nodal vector. The singular branch returns its declared status and asserts nothing about solvability of its right-hand side.

3.1step 1.1step 1.2step 2.1step 2.2∎

Steps 1.1–2.2 prove the success claim and the stated singular-matrix limit.

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