Download this article
 Download this article For screen
For printing
Recent Issues

Volume 17
Issue 4, 1127–1500
Issue 3, 757–1126
Issue 2, 379–756
Issue 1, 1–377

Volume 16, 10 issues

Volume 15, 8 issues

Volume 14, 8 issues

Volume 13, 8 issues

Volume 12, 8 issues

Volume 11, 8 issues

Volume 10, 8 issues

Volume 9, 8 issues

Volume 8, 8 issues

Volume 7, 8 issues

Volume 6, 8 issues

Volume 5, 5 issues

Volume 4, 5 issues

Volume 3, 4 issues

Volume 2, 3 issues

Volume 1, 3 issues

The Journal
About the Journal
Editorial Board
Editors’ Interests
Submission Guidelines
Submission Form
Policies for Authors
Ethics Statement
ISSN: 1948-206X (e-only)
ISSN: 2157-5045 (print)
Author Index
To Appear
Other MSP Journals
Partial regularity for Navier–Stokes and liquid crystals inequalities without maximum principle

Gabriel S. Koch

Vol. 16 (2023), No. 7, 1701–1744

In 1985, V. Scheffer discussed partial regularity results for what he called solutions to the Navier–Stokes inequality. These maps essentially satisfy the incompressibility condition as well as the local and global energy inequalities and the pressure equation which may be derived formally from the Navier–Stokes system of equations, but they are not required to satisfy the Navier–Stokes system itself.

We extend this notion to a system considered by Fang-Hua Lin and Chun Liu in the mid 1990s related to models of the flow of nematic liquid crystals, which include the Navier–Stokes system when the director field d is taken to be zero. In addition to an extended Navier–Stokes system, the Lin–Liu model includes a further parabolic system which implies an a priori maximum principle for d which they use to establish partial regularity (specifically, 𝒫1(𝒮) = 0) of solutions.

For the analogous inequality one loses this maximum principle, but here we nonetheless establish the partial regularity result 𝒫92+δ(𝒮) = 0, so that in particular the putative singular set 𝒮 has space- time Lebesgue measure zero. Under an additional assumption on d for any fixed value of a certain parameter σ (5,6) — which for σ = 6 reduces precisely to the boundedness of d used by Lin and Liu — we obtain the same partial regularity (𝒫1(𝒮) = 0) as do Lin and Liu. In particular, we recover the partial regularity result (𝒫1(𝒮) = 0) of Caffarelli–Kohn–Nirenberg [1982] for suitable weak solutions of the Navier–Stokes system, and we verify Scheffer’s assertion that the same holds for solutions of the weaker inequality as well.

We remark that the proofs of partial regularity both here and in the work of Lin and Liu largely follow the proof in Caffarelli–Kohn–Nirenberg, which in turn used many ideas from an earlier work of Scheffer [1975].

Navier–Stokes, liquid crystals, partial regularity
Mathematical Subject Classification
Primary: 35A21, 35B65, 35D30, 35G50, 35Q35
Received: 28 October 2021
Accepted: 7 January 2022
Published: 21 September 2023
Gabriel S. Koch
Department of Mathematics
University of Sussex
United Kingdom

Open Access made possible by participating institutions via Subscribe to Open.