45 research outputs found

    An anisotropic regularity condition for the 3D incompressible Navier-Stokes equations for the entire exponent range

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    We show that a suitable weak solution to the incompressible Navier-Stokes equations on R3×(−1,1){\mathbb{R}^3\times(-1,1)} is regular on R3×(0,1]\mathbb{R}^3\times(0,1] if ∂3u\partial_3 u belongs to M2p/(2p−3),α((−1,0);Lp(R3))M^{2p/(2p-3),\alpha } ((-1,0);L^p (\mathbb{R}^3 )) for any α>1\alpha >1 and p∈(3/2,∞)p\in (3/2,\infty), which is a logarithmic-type variation of a Morrey space in time. For each α>1\alpha >1 this space is, up to a logarithm, critical with respect to the scaling of the equations, and contains all spaces Lq((−1,0);Lp(R3))L^q ((-1,0);L^p (\mathbb{R}^3 )) that are subcritical, that is for which 2/q+3/p<22/q+3/p<2.Comment: 10 page

    Phase transitions in the fractional three-dimensional Navier-Stokes equations

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    The fractional Navier-Stokes equations on a periodic domain [0, L]3[0,\,L]^{3} differ from their conventional counterpart by the replacement of the −νΔu-\nu\Delta\mathbf{u} Laplacian term by νsAsu\nu_{s}A^{s}\mathbf{u}, where A=−ΔA= - \Delta is the Stokes operator and νs=νL2(s−1)\nu_{s} = \nu L^{2(s-1)} is the viscosity parameter. Four critical values of the exponent ss have been identified where functional properties of solutions of the fractional Navier-Stokes equations change. These values are: s=13s=\frac{1}{3}; s=34s=\frac{3}{4}; s=56s=\frac{5}{6} and s=54s=\frac{5}{4}. In particular, in the fractional setting we prove an analogue of one of the Prodi-Serrin regularity criteria (s>13s > \frac{1}{3}), an equation of local energy balance (s≥34s \geq \frac{3}{4}) and an infinite hierarchy of weak solution time averages (s>56s > \frac{5}{6}). The existence of our analogue of the Prodi-Serrin criterion for s>13s > \frac{1}{3} suggests that the convex integration schemes that construct H\"older-continuous solutions with epochs of regularity for s<13s < \frac{1}{3} are sharp with respect to the value of ss
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