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A Criterion for Uniqueness of Lagrangian Trajectories for Weak Solutions of the 3D Navier-Stokes Equations
Authors:James C. Robinson and Witold Sadowski
Affiliation:(1) Mathematics Institute, University of Warwick, Coventry, CV4 7AL, UK;(2) Faculty of Mathematics, Informatics and Mechanics, University of Warsaw, Banacha 2, 02-097 Warszawa, Poland
Abstract:Foias, Guillopé, & Temam showed in 1985 that for a given weak solution $${uin L^infty(0,T;L^2)cap L^2(0,T;H^1)}$$ of the three-dimensional Navier-Stokes equations on a domain Ω, one can define a ‘trajectory mapping’ $${Phi:Omegatimes[0,T]rightarrowOmega}$$ that gives a consistent choice of trajectory through each initial condition $${ainOmega,,xi_a(t)=Phi(a,t)}$$ , and that respects the volume-preserving property one would expect for smooth flows. The uniqueness of this mapping is guaranteed by the theory of renormalised solutions of non-smooth ODEs due to DiPerna & Lions. However, this is a distinct question from the uniqueness of individual particle trajectories. We show here that if one assumes a little more regularity for u than is known to be the case, namely that $${uin L^{6/5}(0,T;L^infty(Omega))}$$ , then the particle trajectories are unique and C 1 in time for almost every choice of initial condition in Ω. This degree of regularity is more than can currently be guaranteed for weak solutions ($${uin L^1(0,T;L^infty)}$$) but significantly less than that known to ensure that u is regular ($${uin L^2(0,T;L^infty))}$$ . We rely heavily on partial regularity results due to Caffarelli, Kohn, & Nirenberg and Ladyzhenskaya & Seregin.
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