2016
DOI: 10.1016/j.jmaa.2016.03.037
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Navier–Stokes equations with vorticity in Besov spaces of negative regular indices

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Cited by 19 publications
(6 citation statements)
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“…In particular, if θ = Const., then system (1.1) reduces to the classical Navier-Stokes system which describes the motion of incompressible viscous fluid flows and has been extensively studied by many authors; see [18][19][20][21][22][23][24] and the references therein. In addition to this, the reader is referred to [25][26][27][28][29] to find more results about the related fluid flow equations.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, if θ = Const., then system (1.1) reduces to the classical Navier-Stokes system which describes the motion of incompressible viscous fluid flows and has been extensively studied by many authors; see [18][19][20][21][22][23][24] and the references therein. In addition to this, the reader is referred to [25][26][27][28][29] to find more results about the related fluid flow equations.…”
Section: Introductionmentioning
confidence: 99%
“…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%
“…Thereafter, the regularity problem for the 3D NSEs is solved provided ωL1false(0,T;BMOfalse)$$ \omega \in {L}&#x0005E;1\left(0,T; BMO\right) $$ in [14] and ωLpfalse(0,T;Lqfalse),0.30em2p+3q2,0.30em1p<$$ \omega \in {L}&#x0005E;p\left(0,T;{L}&#x0005E;q\right),\kern0.30em \frac{2}{p}&#x0002B;\frac{3}{q}\le 2,\kern0.30em 1\le p&lt;\infty $$ in [15], and provided two components of vorticity trueω˜=false(ω1,ω2,0false)$$ \tilde{\omega}&#x0003D;\left({\omega}_1,{\omega}_2,0\right) $$ satisfy condition () in [16], and trueω˜L1false(0,T;BMOfalse)$$ \tilde{\omega}\in {L}&#x0005E;1\left(0,T; BMO\right) $$ in [17]. For more advances, we refer to [18–24].…”
Section: Introductionmentioning
confidence: 99%
“…From the scaling point of view, is important in the sense that if u is a solution of , then u λ ( x , t )= λu ( λx , λ 2 t ) with λ >0 is a parameter of solutions of ; moreover, false‖uλfalse‖Lpfalse(0,t;Lqfalse(R3false)false)=false‖ufalse‖Lpfalse(0,λT;Lqfalse(R3false)false),0.1em0.1emif and only if0.8em0.1em2p+3q=1. Regularity criterion was later generalized by Beir truea˜o da Veiga to be u0.3emor0.3emωtrue=def×uLpfalse(0,T;Lqfalse(R3false)false),1em2p+3q=2,1em32q. The Prodi‐Serrin conditions was improved from classical Lebesgue spaces larger Besov spaces by Kozono‐Shimada: uL21rfalse(0,T;trueḂ,rfalse(R3false)false),1em0<r<1. Zhang and Yang extended and simultaneously as rightleftuorωL22r(0,T;Ḃ,r(double-struckR3)…”
Section: Introductionmentioning
confidence: 99%