2019
DOI: 10.1016/j.aml.2019.04.012
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Blow-up criteria for the 3D liquid crystal flows involving two velocity components

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Cited by 5 publications
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“…then the solution (u, d) can be extended smoothly beyond T. Later Zhao et al 13 improved the above regularity criterion (1.2) to the following…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…then the solution (u, d) can be extended smoothly beyond T. Later Zhao et al 13 improved the above regularity criterion (1.2) to the following…”
Section: Introductionmentioning
confidence: 99%
“…That is, if 0Tfalse‖u3false‖Lpq+false‖dfalse‖Lpqnormaldt<,0.3emwith0.3em3p+2q34+12p,0.3em103p,$$ {\int}_0&#x0005E;T{\left\Vert {u}_3\right\Vert}_{L&#x0005E;p}&#x0005E;q&#x0002B;{\left\Vert \nabla d\right\Vert}_{L&#x0005E;p}&#x0005E;q\mathrm{d}t&lt;\infty, \kern0.3em with\kern0.3em \frac{3}{p}&#x0002B;\frac{2}{q}\le \frac{3}{4}&#x0002B;\frac{1}{2p},\kern0.3em \frac{10}{3}\le p, $$ then the solution false(u,dfalse)$$ \left(u,d\right) $$ can be extended smoothly beyond T$$ T $$. Later Zhao et al 13 improved the above regularity criterion () to the following 0Tfalse‖uhfalse‖Lpqnormaldt<,0.3emwith0.3em3p+2q12,0.3em6p,$$ {\int}_0&#x0005E;T{\left\Vert {u}_h\right\Vert}_{L&#x0005E;p}&#x0005E;q\mathrm{d}t&lt;\infty, \kern0.3em with\kern0.3em \frac{3}{p}&#x0002B;\frac{2}{q}\le \frac{1}{2},\kern0.3em 6\le p\le \infty, $$ where uh=false(u1,u2false)$$ {u}_h&#x0003D;\left({u}_1,{u}_2\right) $$ is the horizontal component of velocity. And Yuan and Li 10 generalized the regularity cri...…”
Section: Introductionmentioning
confidence: 99%