A strengthening of the energy inequality for the Leray-Hopf solutions of the 3D periodic Navier-Stokes equations

TL;DR

This paper derives a strengthened energy inequality for Leray-Hopf solutions of the 3D periodic Navier-Stokes equations, extending the classical energy inequality with a more general function , which could improve understanding of solution behavior.

Contribution

The authors establish a generalized energy inequality involving an arbitrary absolutely continuous, non-decreasing function , providing a new tool for analyzing Leray-Hopf solutions of the 3D Navier-Stokes equations.

Findings

The inequality holds for all Leray-Hopf points and times.

It generalizes the classical energy inequality with a flexible function .

Potential applications in regularity and stability analysis.

Abstract

In present note we establish the following inequality for the the Leray-Hopf solutions of the 3-D $\Omega$-periodic Navier-Stokes Equations: \[\phi(|u(t)|^2)-\phi(|u(t_0)|^2)\le 2\int_{t_0}^{t}\phi'(|u(\tau)|^2) [-\nu|A^{1/2}u(\tau)|^2+(g(\tau),u(\tau))]\,d\tau\] for all $t_0$ Leray-Hopf points, $t\ge t_0$, and $\phi:\mathbb{R}_{+}\to\mathbb{R}$ is an absolutely continouos non-decreasing function with bounded derivative. %with $\phi'(\xi)\ge0$ for all $\xi>0$. Here $(\cdot,\cdot)$ and $|\cdot|$ is correspondingly the $L^2$ inner product and the $L^2$ norm on $\Omega$, and $A$ is the Stokes operator.