Abstract
The issue of why computational resolution in Navier-Stokes turbulence is so hard to achieve is addressed. It is shown that Navier-Stokes solutions can potentially behave differently in two distinct regions of space-time where is comprised of a union of disjoint space-time `anomalies'. Large values of $|\nabla\bom|$ dominate , which is consistent with the formation of vortex sheets or tightly-coiled filaments. The local number of degrees of freedom needed to resolve the regions in satisfies $$\mathcal{N}^{\pm}(\bx, t)\lessgtr c_{\pm}\mathcal{R}_{u}^{3}$$ where is a Reynolds number dependent on the local velocity field $u(\bx, t)$.
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