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Ann Univ Ferrara (2009) 55:195–197 DOI 10.1007/s11565-009-0081-5 Reinhard Farwig · Jiri ˇ Neustupa · Patrick Penel Published online: 17 October 2009 © Università degli Studi di Ferrara 2009 The mathematical theory of the Navier–Stokes equations poses—since the pioneering work of Jean Leray in 1934—a famous open problem for instationary solutions in three dimensions: It is unknown whether the so-called weak solution which does exist globally in time is regular or smooth for all times if the initial data is regular and large. Analogously, it is open whether a regular solution which can be constructed on a sufficiently small time interval does exist globally in time. Due to its utmost importance for the theory of nonlinear partial differential equations and applications in fluid mechanics this open problem is one of the seven Millennium Prize Problems of Clay Mathematics Institute, formulated in 2000. It is well-known that, given a domain ⊂ R , a time interval (0, T ), an external 2 2 force field f ∈ L on × (0, T ) and an initial value u ∈ L , there exists at least one weak solution in the energy class (the Leray–Hopf class) ∞ 2 2 1
ANNALI DELL'UNIVERSITA' DI FERRARA – Springer Journals
Published: Oct 17, 2009
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