Shape Differentiation and Anisotropy Onset of Quadratic Invariant-Manifold Jets in Surface Navier–Stokes Flow

For a C1 family of smooth closed genus-zero surfaces, we study the quadratic normal jet of unforced surface Navier–Stokes flow near the zero equilibrium. Under an isolated rank-three Riesz slow block and a three-weight slow–fast gap, local C2 invariant graphs share this quotient-valued second derivative after tangent-input identification, without requiring uniqueness of the full graph. A fixed-complement representative is C1 in shape in a bilinear Sobolev-operator norm with infinite-dimensional output. An exact covariance law handles admissible comparisons, including spatial transports with derivative loss. At the unit sphere, the jet vanishes. For symmetric affine deformations, its first variation is a degree-three spherical-harmonic tensor with coefficient −1/(45ν), vanishing exactly for scalar deformation matrices. For each fixed nonscalar D, the jet is therefore nonzero for all sufficiently small 0<|δ|<δ0(D). The onset is local and non-quantitative; no explicit value of δ0(D) is obtained.

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Publication Details

Journal
Mathematics
Published
2026-11-04
DOI
https://doi.org/10.3390/math14214044
Primary Topic
Navier-Stokes equation solutions
Type
article
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article

Shape Differentiation and Anisotropy Onset of Quadratic Invariant-Manifold Jets in Surface Navier–Stokes Flow

Ibrahim S. Elshazly, Amr M. Y. Abdelaty, Hesham A. Abdelghafar
Mathematics
Navier-Stokes equation solutions
article

Shape Differentiation and Anisotropy Onset of Quadratic Invariant-Manifold Jets in Surface Navier–Stokes Flow

Ibrahim S. Elshazly, Amr M. Y. Abdelaty, Hesham A. Abdelghafar
article en

Abstract

For a C1 family of smooth closed genus-zero surfaces, we study the quadratic normal jet of unforced surface Navier–Stokes flow near the zero equilibrium. Under an isolated rank-three Riesz slow block and a three-weight slow–fast gap, local C2 invariant graphs share this quotient-valued second derivative after tangent-input identification, without requiring uniqueness of the full graph. A fixed-complement representative is C1 in shape in a bilinear Sobolev-operator norm with infinite-dimensional output. An exact covariance law handles admissible comparisons, including spatial transports with derivative loss. At the unit sphere, the jet vanishes. For symmetric affine deformations, its first variation is a degree-three spherical-harmonic tensor with coefficient −1/(45ν), vanishing exactly for scalar deformation matrices. For each fixed nonscalar D, the jet is therefore nonzero for all sufficiently small 0<|δ|<δ0(D). The onset is local and non-quantitative; no explicit value of δ0(D) is obtained.

MathematicsVol. 14(21)
King Saud University (SA)
Openalex Percentile: Top 11%
Navier-Stokes equation solutions
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