For , the derivatives are and . Its endpoint values are and , so it satisfies both the ordinary differential equation and the boundary conditions. Moreover any solution of has the form ; the boundary conditions force and . Thus the unique solution of the boundary value problem is
The endpoint boundary conditions areThe finite difference equation can be written . Set . Then , so . Summing from to givesUsing and yields , hence . ThereforeThis also covers , where there are no interior equations. Uniqueness follows because the difference of two solutions has zero second finite difference, hence is linear in , and vanishes at both endpoints. This is an exact finite difference solution for constant second derivative: the method is exact at the nodes here because the centered second finite difference differentiates this quadratic polynomial exactly.
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