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Finite time blowup for an averaged three-dimensional Navier-Stokes equation
JOURNAL OF THE AMERICAN MATHEMATICAL SOCIETY, no. 3 (2016): 601-674
摘要
The Navier-Stokes equation on the Euclidean space $\mathbf{R}^3$ can be expressed in the form $\partial_t u = \Delta u + B(u,u)$, where $B$ is a certain bilinear operator on divergence-free vector fields $u$ obeying the cancellation property $\langle B(u,u), u\rangle=0$ (which is equivalent to the energy identity for the Navier-Stokes e...更多
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