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A boundary-aware discrete maximum principle for the θ scheme

Statement

On the finite two-dimensional rectangular Dirichlet grid of Fully discrete θ heat finite-difference scheme, suppose θ∈[0,1], the source is zero, and

Δt(1−θ)(κxhx2+κyhy2)≤12.

Then every numerical interior value at every time level lies between the minimum and maximum of all initial and prescribed boundary values. In particular, with homogeneous boundary rows and θ=1/2, this maximum-principle condition is Δt(κx/hx2+κy/hy2)≤1, a stricter sufficient condition than the unconditional weighted L2 stability for the same homogeneous problem proved in Unconditional weighted L2 stability for θ at least one half.

Facts & Assumptions

Given: A finite two-dimensional rectangular Dirichlet grid, κx,κy>0, Δt>0, θ∈[0,1], zero source, initial values, and prescribed boundary rows at every time level as in Fully discrete θ heat finite-difference scheme.

[F1]

Fully discrete θ heat finite-difference scheme defines the exact Dirichlet neighbor rows and the centered θ update. Put μx=Δtκx/hx2, μy=Δtκy/hy2.

[F2]

Unique solvability of an implicit θ heat step: each implicit interior step has a unique solution for its known right-hand side and prescribed boundary data.

[F3]

Unconditional weighted L2 stability for θ at least one half: for θ∈[1/2,1] and homogeneous Dirichlet data, the θ step is weighted-L2 contractive for every positive time step.

Proof

1.1F1givenalgebra

Put s=μx+μy and let Vk denote the full grid values, equal to Uk in the interior and Bk on the boundary. At each interior node the zero-source update is (1+2θs)Uijn+1−θμx(Vi+1,jn+1+Vi−1,jn+1)−θμy(Vi,j+1n+1+Vi,j−1n+1)=[1−2(1−θ)s]Uijn+(1−θ)μx(Vi+1,jn+Vi−1,jn)+(1−θ)μy(Vi,j+1n+Vi,j−1n). The right side is known; its center coefficient is nonnegative by the stated condition, and its neighbor coefficients are nonnegative because θ∈[0,1] and μx,μy>0. Thus it is nonnegative whenever the old interior and boundary values are nonnegative.

1.2F1F2givenalgebra

Let W be the unique interior solution of the implicit system with nonnegative right-hand side and nonnegative future boundary data, whose existence is [F2]. If an interior value attained a negative minimum Wij<0, then every adjacent interior or boundary value would be at least Wij, so Wij+θμx(2Wij−Wi+1,j−Wi−1,j)+θμy(2Wij−Wi,j+1−Wi,j−1)≤Wij<0. This is the corresponding component of the nonnegative right-hand side, a contradiction. Hence W≥0; for θ=0 the same inequality reduces to Wij<0 and gives the contradiction directly.

2.1F1step 1.1step 1.2algebra

The zero-source scheme is linear. Let M0 and m0 be respectively the maximum and minimum of the finite collection of initial and prescribed boundary values at all time levels. The constant grid with interior and boundary values M0 solves the zero-source scheme with constant boundary rows M0, since every centered second difference of a constant is zero. Subtracting the numerical solution U gives a solution with initial values M0−U0≥0 and boundary rows M0−Bn≥0. Induction using steps 1.1–1.2 gives U≤M0. Likewise, subtracting the constant grid with interior and boundary values m0 from U gives initial values U0−m0≥0 and boundary rows Bn−m0≥0, so induction gives U≥m0. Thus m0≤Uijn≤M0 at every interior node and time level; the prescribed boundary nodes satisfy the same bounds by definition.

3.1F3givenalgebra∎

In the homogeneous-boundary case at θ=1/2, the stated sufficient maximum-principle restriction reduces to Δt(κx/hx2+κy/hy2)≤1. By [F3] weighted L2 stability holds for every Δt>0 under the same zero-boundary setup. Thus the maximum-principle condition is a stricter sufficient condition; this comparison makes no claim that the maximum principle fails outside it.

Remarks

For θ=1 the restriction is automatic; the precise θ=1/2 comparison with weighted L2 stability is proved in step 3.1. This theorem is specific to the centered rectangular Dirichlet rows stated above. No choice axiom is used.

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