PreprintCC0arXiv
Stability threshold of the Poiseuille flow in 2D Navier-Stokes Boussinesq equations
Abstract
We study the transition threshold problem for the 2D Navier--Stokes Boussinesq equations around the Poiseuille flow on three domains: 𝕋 × ℝ, 𝕋 × [0, ∞), and 𝕋 × [−1, 1]. More precisely, we prove that if the initial perturbations of the vorticity and the temperature are assumed size O(min{νfr34,μfr34,ν−fr14μ}) and O(min{νfr94,μfr94}) in an anisotropic Sobolev space respectively, then for the solution to this system, its size remains so for all time, and the nonlinear enhanced dissipation persists with a rate proportional to O(min{νfr12,μfr12}).
Related
- Enhanced dissipation and stability threshold for the Navier--Stokes equations near Poiseuille flow
- Stability threshold of the Couette flow in 2D Navier-Stokes Boussinesq equations on 𝕋 × [−1, 1] and ℝ × [−1, 1]
- The stability threshold for Boussinesq equations around stratified Couette flow with unequal viscosity and thermal diffusivity on 𝕋×ℝ2
- Stability threshold for 3D Boussinesq equations with rotation near the Couette flow and vertical stratified temperature
- On the Sobolev stability threshold for 3D Navier-Stokes equations with rotation near the Couette flow
BibTeX
@misc{zhang2026stability,
title = {{Stability threshold of the Poiseuille flow in 2D Navier-Stokes Boussinesq equations}},
author = {Nangao Zhang},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.07598},
eprint = {2610.07598},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.07598},
note = {CC0},
}
RIS
TY - UNPB
TI - Stability threshold of the Poiseuille flow in 2D Navier-Stokes Boussinesq equations
AU - Nangao Zhang
PY - 2026
DA - 2026/10/06
PB - arXiv
DO - 10.48550/arxiv.2610.07598
UR - https://arxiv.org/abs/2610.07598
AB - We study the transition threshold problem for the 2D Navier--Stokes Boussinesq equations around the Poiseuille flow on three domains: 𝕋 × ℝ, 𝕋 × [0, ∞), and 𝕋 × [−1, 1]. More precisely, we prove that if the initial perturbations of the vorticity and the temperature are assumed size O(min{ν^fr34,μ^fr34,ν^−fr14μ}) and O(min{ν^fr94,μ^fr94}) in an anisotropic Sobolev space respectively, then for the solution to this system, its size remains so for all time, and the nonlinear enhanced dissipation persists with a rate proportional to O(min{ν^fr12,μ^fr12}).
ER -