Global regularity for three-dimensional incompressible Euler
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For every divergence-free Schwartz vector field \(u_0\in\mathcal S(\mathbb R^3;\mathbb R^3)\), the maximal classical solution of \[ \partial_tu+(u\cdot\nabla)u=-\nabla p,\qquad \nabla\cdot u=0,\qquad u(\cdot,0)=u_0 \] exists for all \(t\ge0\) and belongs to \(C^\infty(\mathbb R^3\times[0,\infty))\).Notes
The problem asks whether every divergence-free Schwartz initial velocity field on gives rise to a classical solution of the incompressible Euler equations that stays smooth for all . Unlike Navier–Stokes there is no viscous term, and the mechanism of concern is vortex stretching. The question has no single point of origin: it crystallized gradually from the early PDE theory of the Euler equations, roughly in the 1930s.
The classical Beale–Kato–Majda criterion shows that blow-up can occur only if the time integral of diverges, so any singularity must be accompanied by unbounded vorticity growth [BealeKatoMajda1984Euler]; the surrounding blow-up literature is surveyed in [Chae2007EulerBlowupSurvey]. More recently, rigorous finite-time singularities have been constructed for solutions below the classical smoothness threshold, including regimes [ChenHou2025EulerSingularities], sharpening the sense in which the smooth problem is critical.
For smooth finite-energy data, however, neither blow-up nor global regularity has been proved, and the problem is open in both directions.
References (3)
- [BealeKatoMajda1984Euler]
Remarks on the breakdown of smooth solutions for the 3-D Euler equations
Open ↗1984 · misc
- [Chae2007EulerBlowupSurvey]
Incompressible Euler equations: the blow-up problem and related results
Open ↗2008 · misc
- [ChenHou2025EulerSingularities]
Finite time singularities to the 3D incompressible Euler equations for solutions in C^( R^3) C^(1,) L^2
Open ↗2025 · misc
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