2017
DOI: 10.1016/j.jde.2017.05.016
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Extension criterion via partial components of vorticity on strong solutions to the Navier–Stokes equations in higher dimensions

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Cited by 3 publications
(6 citation statements)
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“…This result indicates that, among the nfalse(n1false)2 components of the vorticity, []n2 components are negligible for the criterion whether the time local solutions can be extended beyond the critical time, which can be viewed as the generalization to the higher dimensional case of Chae and Choe . On the other hand, the author suggested difficulties in relaxing to trueB˙,0.1em0 like in the work of Zhang and Chen (see remark 2.2 (ii), p. 4012 in the work of Tsurumi). The purpose of this paper is to give an affirmative answer to this problem.…”
Section: Introductionmentioning
confidence: 90%
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“…This result indicates that, among the nfalse(n1false)2 components of the vorticity, []n2 components are negligible for the criterion whether the time local solutions can be extended beyond the critical time, which can be viewed as the generalization to the higher dimensional case of Chae and Choe . On the other hand, the author suggested difficulties in relaxing to trueB˙,0.1em0 like in the work of Zhang and Chen (see remark 2.2 (ii), p. 4012 in the work of Tsurumi). The purpose of this paper is to give an affirmative answer to this problem.…”
Section: Introductionmentioning
confidence: 90%
“…Consequently, one may verify that X ( t ) is a monotonically nondecreasing function. Our next target is to show that, under the assumption , it holds true limtTX(t)Cu0,T,X(T0)<. Thanks to ▽· u = 0 and the definition of ω , we have uk=(Δ)1i=1niωik, which along with yields u˜L2CuL2,normalΛsu˜L2CnormalΛsuL2. Noticing the following fact (see (3.6) in the work of Tsurumi) ju˜k=scriptRji=1nscriptRiω˜ik, where Rl=lfalse(normalΔfalse)12, l = 1,2,…, n denote the classical Riesz transforms, we thus have u˜B˙…”
Section: The Proof Of Theoremmentioning
confidence: 97%
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“…in [15], and provided two components of vorticity ω = (𝜔 1 , 𝜔 2 , 0) satisfy condition (1.2) in [16], and ω ∈ L 1 (0, T; BMO) in [17]. For more advances, we refer to [18][19][20][21][22][23][24]. Very recently, for system (1.1) with p ≠ 2, there have been studied the regularity criteria in terms of velocity or direction of vorticity in [8,[25][26][27][28].…”
Section: Introductionmentioning
confidence: 99%