Long-wave instability of periodic shear flows for the 2D Navier-Stokes equations

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Main Authors: Colombo, Maria, Dolce, Michele, Montalto, Riccardo, Ventura, Paolo
Format: Preprint
Published: 2025
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author Colombo, Maria
Dolce, Michele
Montalto, Riccardo
Ventura, Paolo
author_facet Colombo, Maria
Dolce, Michele
Montalto, Riccardo
Ventura, Paolo
contents In 1959, Kolmogorov proposed to study the instability of the shear flow $(\sin(y),0)$ in the vanishing viscosity regime in tori $\mathbb{T}_α\times \mathbb{T}$. This question was later resolved by Meshalkin and Sinai. We extend the problem to general shear flows $(U(y),0)$ and show that every $U(y)$ exhibits long-wave instability whenever $\|\partial_y^{-1} U\|_{L^2} > ν$ and $α\ll ν$, with $ν$ being the kinematic viscosity. This instability mechanism confirms previous findings by Yudovich in 1966, supported also by several numerical results, and is established through two independent approaches: one via the construction of Kato's isomorphism and one via normal forms. Unlike in many other applications of the latter methods, both proofs deal with the presence of a delicate term in the linearized operator that becomes singular as $α$ approaches $0$.
format Preprint
id arxiv_https___arxiv_org_abs_2509_18070
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Long-wave instability of periodic shear flows for the 2D Navier-Stokes equations
Colombo, Maria
Dolce, Michele
Montalto, Riccardo
Ventura, Paolo
Analysis of PDEs
Fluid Dynamics
76D05, 76D33, 35Q30, 35Q35, 35P15
In 1959, Kolmogorov proposed to study the instability of the shear flow $(\sin(y),0)$ in the vanishing viscosity regime in tori $\mathbb{T}_α\times \mathbb{T}$. This question was later resolved by Meshalkin and Sinai. We extend the problem to general shear flows $(U(y),0)$ and show that every $U(y)$ exhibits long-wave instability whenever $\|\partial_y^{-1} U\|_{L^2} > ν$ and $α\ll ν$, with $ν$ being the kinematic viscosity. This instability mechanism confirms previous findings by Yudovich in 1966, supported also by several numerical results, and is established through two independent approaches: one via the construction of Kato's isomorphism and one via normal forms. Unlike in many other applications of the latter methods, both proofs deal with the presence of a delicate term in the linearized operator that becomes singular as $α$ approaches $0$.
title Long-wave instability of periodic shear flows for the 2D Navier-Stokes equations
topic Analysis of PDEs
Fluid Dynamics
76D05, 76D33, 35Q30, 35Q35, 35P15
url https://arxiv.org/abs/2509.18070