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Dynamics near the subcritical transition of the 3D Couette flow II: Above threshold case

Jacob Bedrossian, Pierre Germain, Nader Masmoudi

TL;DR

The paper advances the mathematical understanding of the 3D Navier–Stokes dynamics near plane Couette flow in the subcritical regime by establishing that, above a sharp threshold ε ≲ Re^{-2/3-δ}, small disturbances persist up to time t ~ c0 ε^{-1} and evolve toward the class of streaks due to lift-up, with rapid damping of nonzero streamwise modes by mixing-enhanced dissipation. It introduces a refined Gevrey-based energy framework and a near-Lagrangian coordinate transform to control the growth from lift-up while capturing the secondary instability pathway leading to streak breakdown. A detailed bootstrap argument bounds high-norm quantities for the velocity components, the coordinate system, and the auxiliary g,C variables, balancing nonlinear interactions via a toy-model-informed norm design and paraproduct decomposition. The results support the conventional narrative lift-up → streak growth → streak breakdown as a generic route to transition near the stability threshold, extending previous subcritical analyses to the above-threshold regime and clarifying the role of regularity and enhanced dissipation in sustaining transient large-amplitude streaks. Applicability to high-Re turbulence near threshold is reinforced by the explicit ε–ν balance and the explicit time scales τ_ED ∼ ν^{-1/3} and τ_NL ∼ ε^{-1/2} that govern the nonlinear-to-dissipative competition.

Abstract

This is the second in a pair of works which study small disturbances to the plane, periodic 3D Couette flow in the incompressible Navier-Stokes equations at high Reynolds number $\textbf{Re}$. In this work, we show that there is constant $0 < c_0 \ll 1$, independent of $\textbf{Re}$, such that sufficiently regular disturbances of size $ε\lesssim \textbf{Re}^{-2/3-δ}$ for any $δ> 0$ exist at least until $t = c_0ε^{-1}$ and in general evolve to be $O(c_0)$ due to the lift-up effect. Further, after times $t \gtrsim \textbf{Re}^{1/3}$, the streamwise dependence of the solution is rapidly diminished by a mixing-enhanced dissipation effect and the solution is attracted back to the class of "2.5 dimensional" streamwise-independent solutions (sometimes referred to as "streaks"). The largest of these streaks are expected to eventually undergo a secondary instability at $t \approx ε^{-1}$. Hence, our work strongly suggests, for all (sufficiently regular) initial data, the genericity of the "lift-up effect $\Rightarrow$ streak growth $\Rightarrow$ streak breakdown" scenario for turbulent transition of the 3D Couette flow near the threshold of stability forwarded in the applied mathematics and physics literature.

Dynamics near the subcritical transition of the 3D Couette flow II: Above threshold case

TL;DR

The paper advances the mathematical understanding of the 3D Navier–Stokes dynamics near plane Couette flow in the subcritical regime by establishing that, above a sharp threshold ε ≲ Re^{-2/3-δ}, small disturbances persist up to time t ~ c0 ε^{-1} and evolve toward the class of streaks due to lift-up, with rapid damping of nonzero streamwise modes by mixing-enhanced dissipation. It introduces a refined Gevrey-based energy framework and a near-Lagrangian coordinate transform to control the growth from lift-up while capturing the secondary instability pathway leading to streak breakdown. A detailed bootstrap argument bounds high-norm quantities for the velocity components, the coordinate system, and the auxiliary g,C variables, balancing nonlinear interactions via a toy-model-informed norm design and paraproduct decomposition. The results support the conventional narrative lift-up → streak growth → streak breakdown as a generic route to transition near the stability threshold, extending previous subcritical analyses to the above-threshold regime and clarifying the role of regularity and enhanced dissipation in sustaining transient large-amplitude streaks. Applicability to high-Re turbulence near threshold is reinforced by the explicit ε–ν balance and the explicit time scales τ_ED ∼ ν^{-1/3} and τ_NL ∼ ε^{-1/2} that govern the nonlinear-to-dissipative competition.

Abstract

This is the second in a pair of works which study small disturbances to the plane, periodic 3D Couette flow in the incompressible Navier-Stokes equations at high Reynolds number . In this work, we show that there is constant , independent of , such that sufficiently regular disturbances of size for any exist at least until and in general evolve to be due to the lift-up effect. Further, after times , the streamwise dependence of the solution is rapidly diminished by a mixing-enhanced dissipation effect and the solution is attracted back to the class of "2.5 dimensional" streamwise-independent solutions (sometimes referred to as "streaks"). The largest of these streaks are expected to eventually undergo a secondary instability at . Hence, our work strongly suggests, for all (sufficiently regular) initial data, the genericity of the "lift-up effect streak growth streak breakdown" scenario for turbulent transition of the 3D Couette flow near the threshold of stability forwarded in the applied mathematics and physics literature.

Paper Structure

This paper contains 165 sections, 38 theorems, 448 equations.

Key Result

Proposition 1.1

Consider the linearized Navier-Stokes equations Let $u_{in}$ be a divergence free vector field with $u_{in} \in H^7$. Then the solution to the linearized Navier-Stokes equations $u(t)$ with initial data $u_{in}$ satisfies the following for some $c \in (0,1/3)$, and the formulas

Theorems & Definitions (61)

  • Proposition 1.1
  • Proposition 1.2: Streak solutions
  • Theorem 1: Above threshold dynamics
  • Remark 1.1
  • Remark 1.2
  • Remark 1.3
  • Remark 1.4
  • Remark 1.5
  • Remark 1.6
  • Lemma 2.1: Local existence and instanteous regularization
  • ...and 51 more