The Millennium Prize problem regarding the global regularity of the 3D incompressible Navier-Stokes equations is traditionally framed within the unbounded continuum domain ℝ3. This paper demonstrates that under a specific, highly rotational axisymmetric initial condition—comprising two counter-propagating vortex rings configured for a head-on topological collision—the continuous equations inevitably develop a singularity in finite time. By utilizing C0∞ bump functions, we construct a strict ℝ3 topology that forces a massive radial expansion and generates an uncontrollable centrifugal force gradient. Through the evaluation of the Calderón-Zygmund singular integral, we prove that the macroscopic Pressure Hessian strictly locks the principal eigenvectors of the strain rate tensor, completely disabling the fluid's non-linear depletion mechanism. With the topological alignment mathematically preserved (cos2 α ≈ 1), the application of the Gagliardo-Nirenberg-Sobolev inequality demonstrates that the linear Laplacian dissipation is algebraically decoupled and fundamentally insufficient to arrest the non-linear growth of vortex stretching. The subsequent application of the Beale-Kato-Majda (BKM) theorem mathematically guarantees the divergence of global enstrophy along a hyperbolic trajectory, formally establishing a finite-time blow-up and proving the breakdown of the smooth C∞ continuum model.
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Carlos Mariano Hernández Valdivia (2026) studied this question.
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