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   <subfield code="a">An Example of Finite-time Singularities in the 3d Euler Equations</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[Xinyu He]</subfield>
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   <subfield code="a">Abstract.: Let $$\Omega = {\user2{\mathbb{R}}}^{3} \backslash \overline{B} _{1} (0)$$ be the exterior of the closed unit ball. Consider the self-similar Euler system $$\alpha u + \beta y \cdot \nabla u + u \cdot \nabla u + \nabla p = 0, \quad \hbox{div}\, u = 0 \quad {\hbox{in}} \quad\Omega.$$ Setting α = β = 1/2 gives the limiting case of Leray's self-similar Navier-Stokes equations. Assuming smoothness and smallness of the boundary data on ∂Ω, we prove that this system has a unique solution $$(u,p) \in \user1{\mathcal{C}}^1 (\Omega ;\user2{\mathbb{R}}^3 \times\user2{\mathbb{R}}) $$ , vanishing at infinity, precisely $$u(y) \downarrow 0\quad {\hbox{as}}\quad |y| \uparrow \infty ,\quad {\hbox{with}}\quad u = \user1{\mathcal{O}}(|y|^{ - 1} ),\quad \nabla u = \user1{\mathcal{O}}(|y|^{ - 2} ). $$ The self-similarity transformation is v(x, t) = u(y)/(t* − t)α, y = x/(t* − t)β, where v(x, t) is a solution to the Euler equations. The existence of smooth function u(y) implies that the solution v(x, t) blows up at (x*, t*), x* = 0, t* &lt; + ∞. This isolated singularity has bounded energy with unbounded L 2 − norm of curl v.</subfield>
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   <subfield code="a">Birkhäuser Verlag, Basel, 2006</subfield>
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   <subfield code="a">Euler equations</subfield>
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   <subfield code="a">singular self-similar solutions</subfield>
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   <subfield code="t">Journal of Mathematical Fluid Mechanics</subfield>
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   <subfield code="g">9/3(2007-08-01), 398-410</subfield>
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   <subfield code="t">Journal of Mathematical Fluid Mechanics</subfield>
   <subfield code="d">Birkhäuser-Verlag; www.birkhäuser.ch</subfield>
   <subfield code="g">9/3(2007-08-01), 398-410</subfield>
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   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">Springer special CC-BY-NC licence</subfield>
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