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A one-sided Neumann closure gives only first-order error

Example

Let h=1/N for an integer N≥2, xi=ih, δh2Vi=(Vi+1−2Vi+Vi−1)/h2, and Dh+V0=(V1−V0)/h. The exact solution u(x)=x2 solves −u′′=−2 on (0,1) with u′(0)=0 and u(1)=1. Discretize the interior equation by −δh2Vi=−2 for 1≤i<N, impose the one-sided Neumann row Dh+V0=0, and impose VN=1. The unique grid solution is

Vi=xi2+h(1−xi),

so max⁡0≤i≤N∣Vi−u(xi)∣=h. The boundary residual of the exact samples is Dh+u(0)−u′(0)=h, and the global error is only first order.

Facts & Assumptions

Given: An integer N≥2, h=1/N, xi=ih, the displayed centered second difference and one-sided forward Neumann row, and the stated mixed discrete equations.

[A1]

The grid equations are −δh2Vi=−2 for 1≤i<N, Dh+V0=0, and VN=1.

Verification

1.1givenA1algebra

For the exact samples ui=xi2, Dh+u0=(h2−0)/h=h, whereas u′(0)=0. Thus the imposed Neumann row has residual exactly h.

1.2A1algebra

Define Vi=xi2+h(1−xi). Then V0=h, V1=h, so Dh+V0=0; also VN=1. Since the second difference of the quadratic part is 2 and the second difference of the affine part is 0, −δh2Vi=−2 at every interior node. Hence V satisfies [A1].

2.1A1step 1.2algebra

If two grid solutions existed, their difference d would satisfy δh2di=0 for 1≤i<N, Dh+d0=0, and dN=0. The recurrence says di−di−1 is constant in i; the forward boundary row makes that constant 0, and dN=0 then makes every di=0. Therefore the solution in step 1.2 is unique.

3.1step 1.1step 1.2algebra∎

The error is Vi−ui=h(1−xi). Because 0≤xi≤1, its maximum absolute value is h, attained at i=0. The boundary residual and global error are both first order in h.

Used by

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Dependency tree · 0 levels

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