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Centered advection is consistent and unstable under the CFL bound
Example
Fix . For , use periodic grids , , and , so . Every fixed smooth -periodic solution in the hypotheses of Smooth consistency orders for the five periodic advection stencils has centered residual . Nevertheless the mode has and multiplier , and the centered family has no uniform finite-time power bound, as proved in The nearest-neighbor CFL condition is necessary but not sufficient.
Facts & Assumptions
Given: Fixed and periodic grids , , , with Fourier index .
The centered residual is under the two-sided mesh-ratio and hypotheses of Smooth consistency orders for the five periodic advection stencils.
The centered amplification factor is (Amplification symbols for periodic scalar advection stencils).
For this centered periodic family with , the finite-time power norms are unbounded as (The nearest-neighbor CFL condition is necessary but not sufficient).
Verification
Since , , and the centered factor is . Its squared modulus is , while is constant and .
By [F1], each fixed smooth solution satisfying the theorem's regularity and periodicity hypotheses has residual . By [F3], for every fixed the centered update powers are not uniformly bounded over time levels . Thus this family is consistent on fixed smooth data but fails finite-time power stability because of mesh-dependent high-frequency modes.
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Sources
- Benjamin Seibold, MIT 18.336 Lecture 15, Finite Difference Methods for the One-Way Wave Equation (standard reference, not scraped)