Randomized trial shows a finite upper bound on shear stress in fluid flow, indicating structural limitations in classical formulations.
We demonstrate that the Navier-Stokes existence and smoothness problem is an artifact of the classical continuum formulation rather than a property of fluid flow. The classical formulation defines shear stress as a ratio (Δu/Δx) that diverges as Δx approaches zero. We show that in physical flow, the distance Δx between adjacent coherent sub-streams cannot decrease below a characteristic scale λ_MTT = C₁·D·Re^(−1/2), the Taylor microscale, because sub-stream boundaries are energy-carrying structures with internal organization, not geometric points. Using Material Tensor Theory (MTT) to model the sub-stream structure and Boundary Algebra (BA) to formalize the boundary as a structured object, we establish a finite upper bound on shear stress: τ_max = μ·Δv/λ_MTT. We validate this framework against Direct Numerical Simulation data from Lee and Moser (2015) at Re_τ = 1,000. The DNS confirms that (1) the velocity gradient converges to a finite value (τ_wall) as resolution increases, (2) the shear stress remains within 99% of τ_wall for y⁺ < 2 and within 90% for y⁺ < 5, and (3) the sub-stream scale λ⁺ = 5.0 wall units, derived from the Taylor microscale with C₁ = 0.5, coincides exactly with the classical viscous sublayer edge. Below this scale, the DNS shows constant shear; above it, shear decays through the buffer and log layers. We argue, following Gödel (1931), that the regularity of Navier-Stokes cannot be proved within its own framework because the framework lacks representational capacity for sub-stream structure. The resolution requires a richer formal system in which the question does not arise.
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Avishai Roif (2026) studied this question.
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