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Centered advection is consistent and unstable under the CFL bound

Example

Fix a,P,T>0. For q≥1, use periodic grids Nq=4q, hq=P/Nq, and kq=hq/(2a), so ν=akq/hq=1/2. Every fixed smooth P-periodic solution in the hypotheses of Smooth consistency orders for the five periodic advection stencils has centered residual O(hq). Nevertheless the mode ℓ=q has zℓ=i and multiplier 1−i/2, 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 a,P,T>0 and periodic grids Nq=4q, hq=P/(4q), kq=hq/(2a), with Fourier index ℓ=q.

[F1]

The centered residual is O(h) under the two-sided mesh-ratio and C6 hypotheses of Smooth consistency orders for the five periodic advection stencils.

[F2]

The centered amplification factor is 1−iνS (Amplification symbols for periodic scalar advection stencils).

[F3]

For this centered periodic family with akq/hq=1/2, the finite-time power norms are unbounded as q→∞ (The nearest-neighbor CFL condition is necessary but not sufficient).

Verification

1.1givenF2algebra

Since zℓ=i, Sℓ=1, and the centered factor is 1−i/2. Its squared modulus is 1+1/4=5/4>1, while kq/hq=1/(2a) is constant and hq,kq→0.

2.1F1F3step 1.1∎

By [F1], each fixed smooth solution satisfying the theorem's regularity and periodicity hypotheses has residual O(hq). By [F3], for every fixed T>0 the centered update powers are not uniformly bounded over time levels rkq≤T. 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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