Statement

Let (u,p)(u,p) be an unforced of the three-dimensional Navier–Stokes equations on an open cylinder QQ, with ν>0\nu>0. Its interior satisfies

Hpar1(S(u))=0,\mathcal H^1_{\rm par}(S(u))=0,

where Hpar1\mathcal H^1_{\rm par} is . This is the unforced interior form of the Caffarelli–Kohn–Nirenberg partial regularity theorem.

It is a statement.

Scope

The conclusion is , not emptiness of the singular set. Boundary versions and forced versions require additional hypotheses and estimates. The theorem uses suitability, including its local energy inequality.

References