1987
DOI: 10.1112/jlms/s2-35.2.303
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Decay Results for Weak Solutions of the Navier-Stokes Equations on Rn

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Cited by 303 publications
(281 citation statements)
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“…In this section, we adapt the results in [13] to the particular case where N = 3 and L ≡ Λ + 1 2 acts on the space of divergence free vector fields L 2 (m) defined in (24). Remark that div(Λf) = L div(f), so that Λ preserves the divergence free condition.…”
Section: A Spectrum Of the Operator λmentioning
confidence: 99%
See 1 more Smart Citation
“…In this section, we adapt the results in [13] to the particular case where N = 3 and L ≡ Λ + 1 2 acts on the space of divergence free vector fields L 2 (m) defined in (24). Remark that div(Λf) = L div(f), so that Λ preserves the divergence free condition.…”
Section: A Spectrum Of the Operator λmentioning
confidence: 99%
“…As no external force is applied, it is intuitively clear that all finite-energy solutions of (2) should converge, as time goes to infinity, to the rest state u ≡ 0, p ≡ const. As a matter of fact, if u(x, t) is any global weak solution in L 2 (R 3 ) satisfying the energy inequality, it is known that u(·, t) L 2 → 0 as t → ∞ (see Wiegner [24]). Moreover, if…”
Section: Introductionmentioning
confidence: 99%
“…Note in particular that kuðtÞk 2 ¼ Oðt À1 Þ as t ! y; so the result of [20] suggests that we would need some symmetry condition to find solutions which decay more rapidly than stated in Theorem 1.1. In fact, [16] proves We know (see [2]…”
Section: à1=2àð1à1=rþmentioning
confidence: 99%
“…Esta questão somente foi resolvida (positivamente) 50 anos mais tarde por Kato [6] e subsequentemente também por outros autores [5,9,17]. Vários desenvolvimentos e extensões importantes de (3) vem sendo estabelecidos (ver e.g.…”
Section: Introductionunclassified