Abstract:(A) It is known that among the currently unresolved cases of the axially symmetric Navier-Stokes equations (ASNS), the most relatively tractable one is where the fluid passes the exterior of a cone. In this paper, we investigate this case with Navier total-slip boundary condition. We show that there exists an absolute constant $C_* > 0$ such that if
\[
\sup_{x\in D}r|v_{0,\theta}|\leq C_* \quad\text{and}\quad \int_{D} r v_{0,\theta}(x) \mathrm{d} x = 0,
\] then there exists a unique global bounded strong solution with finite energy. Note that, for the initial velocity, there is neither a size restriction on other components, nor a parity assumption. There are four key ingredients in the proof.
(1) Three new good unknowns are introduced, and a self-closed energy estimate for them is derived.
(2) An elliptic estimate for pressure is established to control boundary terms arising from the boundary condition.
(3) A De Giorgi iteration scheme is applied to establish the boundedness of $rv_\theta$.
(4) A new anisotropic Hardy's inequality is derived for weighted mean-zero functions to overcome the lack of parity of $\boldsymbol{v}$.
(B) Based on (A), we introduce and prove the so-called controlled regularity for the above problem, i.e. for suitable initial data without any smallness assumption, there exists an external force supported away from the axis of symmetry such that the corresponding problem admits a global strong solution. This seems to add a little weight to the regularity scenario for ASNS, since the force is supported away from the axis which is the only place regularity may break down. We also prove that if there exists a solution that blows up in finite time, an unstable blow-up solution must exist.
From: Zijin Li [view email]
[v1]
Sun, 24 May 2026 15:35:34 UTC (379 KB)
[v2]
Tue, 2 Jun 2026 03:09:28 UTC (394 KB)
[v3]
Wed, 1 Jul 2026 07:56:08 UTC (387 KB)
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